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 |
|---|---|---|---|---|---|---|
706.4314 | Domain growth morphology in curvature driven two dimensional coarsening | We study the distribution of domain areas, areas enclosed by domain
boundaries (''hulls''), and perimeters for curvature-driven two-dimensional
coarsening, employing a combination of exact analysis and numerical studies,
for various initial conditions. We show that the number of hulls per unit area,
$n_h(A,t) dA$, wi... | cond-mat.stat-mech | we study the distribution of domain areas areas enclosed by domain boundaries hulls and perimeters for curvaturedriven twodimensional coarsening employing a combination of exact analysis and numerical studies for various initial conditions we show that the number of hulls per unit area n_hat da with enclosed area in th... | [['we', 'study', 'the', 'distribution', 'of', 'domain', 'areas', 'areas', 'enclosed', 'by', 'domain', 'boundaries', 'hulls', 'and', 'perimeters', 'for', 'curvaturedriven', 'twodimensional', 'coarsening', 'employing', 'a', 'combination', 'of', 'exact', 'analysis', 'and', 'numerical', 'studies', 'for', 'various', 'initia... | [-0.15497852213348307, 0.17514559852126188, -0.04381273892573654, 0.03024282350321923, -0.004001502116038937, -0.1098231808730665, 0.024053254121177415, 0.35734181079196736, -0.23606781874046248, -0.2785432445418269, 0.14596940047060325, -0.2848061596885084, -0.08745052382340007, 0.19586869451232294, -0.010268784083306... |
706.4315 | Cutoff Resolvent Estimates and the Semilinear Schr\"odinger Equation | This paper shows how abstract resolvent estimates imply local smoothing for
solutions to the Schr\"odinger equation. If the resolvent estimate has a loss
when compared to the optimal, non-trapping estimate, there is a corresponding
loss in regularity in the local smoothing estimate. As an application, we apply
well-k... | math.AP | this paper shows how abstract resolvent estimates imply local smoothing for solutions to the schrodinger equation if the resolvent estimate has a loss when compared to the optimal nontrapping estimate there is a corresponding loss in regularity in the local smoothing estimate as an application we apply wellknown techni... | [['this', 'paper', 'shows', 'how', 'abstract', 'resolvent', 'estimates', 'imply', 'local', 'smoothing', 'for', 'solutions', 'to', 'the', 'schrodinger', 'equation', 'if', 'the', 'resolvent', 'estimate', 'has', 'a', 'loss', 'when', 'compared', 'to', 'the', 'optimal', 'nontrapping', 'estimate', 'there', 'is', 'a', 'corres... | [-0.02986087258262881, -0.05864421657968016, -0.12665912920031056, 0.1723456954711984, -0.12067394320660367, -0.11696584741103239, -0.04085204915488781, 0.3218157700551995, -0.2919545153733985, -0.2122005889722114, 0.16764477091632654, -0.33212251474695476, -0.15230663090940275, 0.22127673042745427, -0.1162333430818699... |
706.4316 | On Combining Lensing Shear Information from Multiple Filters | We consider the possible gain in the measurement of lensing shear from
imaging data in multiple filters. Galaxy shapes may differ significantly across
filters, so that the same galaxy offers multiple samples of the shear. On the
other extreme, if galaxy shapes are identical in different filters, one can
combine them ... | astro-ph | we consider the possible gain in the measurement of lensing shear from imaging data in multiple filters galaxy shapes may differ significantly across filters so that the same galaxy offers multiple samples of the shear on the other extreme if galaxy shapes are identical in different filters one can combine them to impr... | [['we', 'consider', 'the', 'possible', 'gain', 'in', 'the', 'measurement', 'of', 'lensing', 'shear', 'from', 'imaging', 'data', 'in', 'multiple', 'filters', 'galaxy', 'shapes', 'may', 'differ', 'significantly', 'across', 'filters', 'so', 'that', 'the', 'same', 'galaxy', 'offers', 'multiple', 'samples', 'of', 'the', 'sh... | [-0.056014746581332396, 0.06945733243702065, -0.09732324270309385, 0.0874508639857378, -0.090828532438486, -0.09999945490629575, -0.028489604199288088, 0.4756353050470352, -0.20119493949833675, -0.3729248103608779, 0.024634242740271768, -0.30285922709613217, -0.08634178547259129, 0.1803976902332362, -0.0487660676275098... |
706.4317 | On the Effects of Dissipative Turbulence on the Narrow Emission-Line
Ratios in Seyfert Galaxies | We present a photoionization model study of the effects of micro-turbulence
and dissipative heating on emission lines for number and column densities,
elemental abundances, and ionizations typical for the narrow emission line
regions (NLRs) of Seyfert galaxies. Earlier studies of NLR spectra generally
found good agre... | astro-ph | we present a photoionization model study of the effects of microturbulence and dissipative heating on emission lines for number and column densities elemental abundances and ionizations typical for the narrow emission line regions nlrs of seyfert galaxies earlier studies of nlr spectra generally found good agreement be... | [['we', 'present', 'a', 'photoionization', 'model', 'study', 'of', 'the', 'effects', 'of', 'microturbulence', 'and', 'dissipative', 'heating', 'on', 'emission', 'lines', 'for', 'number', 'and', 'column', 'densities', 'elemental', 'abundances', 'and', 'ionizations', 'typical', 'for', 'the', 'narrow', 'emission', 'line',... | [-0.020847240029949664, 0.12977086225224366, 0.03222825830371296, 0.09112282428594137, -0.012314768467668043, -0.14517887022484802, 0.037669027457013726, 0.4513429459107439, -0.18093594625132342, -0.3183860354941369, 0.0016174877013372304, -0.30311045304040835, 0.0208347666227405, 0.15601532172348181, 0.009848755783370... |
706.4318 | CDF Hot Topics | We present recent CDF results based on approximately 1 fb$^{-1}$ of $p\bar p$
collisions at $\sqrt s = 1.96$ TeV delivered at Fermilab Tevatron. Results
shown include the observation of the $B_s$ oscillation frequency, the first
observation of bottom baryon $\Sigma_b^{(*)\pm}$ states, updates on $B$ hadrons
lifetimes... | hep-ex | we present recent cdf results based on approximately 1 fb1 of pbar p collisions at sqrt s 196 tev delivered at fermilab tevatron results shown include the observation of the b_s oscillation frequency the first observation of bottom baryon sigma_bpm states updates on b hadrons lifetimes and searches for rare decays in t... | [['we', 'present', 'recent', 'cdf', 'results', 'based', 'on', 'approximately', '1', 'fb1', 'of', 'pbar', 'p', 'collisions', 'at', 'sqrt', 's', '196', 'tev', 'delivered', 'at', 'fermilab', 'tevatron', 'results', 'shown', 'include', 'the', 'observation', 'of', 'the', 'b_s', 'oscillation', 'frequency', 'the', 'first', 'ob... | [-0.05781277399341155, 0.2905837880267251, -0.05676246042393388, 0.07588278658447727, -0.038855678386866085, -0.1378532502980482, 0.10415510459232234, 0.2386290676715303, -0.17086993788759555, -0.2256282862095583, -0.08533889026336011, -0.47915314606601195, 0.1135418907919478, 0.10935459647237533, 0.15213103126734495, ... |
706.4319 | Non-Fermi-liquid behavior in nearly ferromagnetic metallic SrIrO3 single
crystals | We report transport and thermodynamic properties of single-crystal SrIrO3 as
a function of temperature T and applied magnetic field H. We find that SrIrO3
is a non-Fermi-liquid metal near a ferromagnetic instability, as characterized
by the following properties: (1) small ordered moment but no evidence for
long-range... | cond-mat.str-el | we report transport and thermodynamic properties of singlecrystal sriro3 as a function of temperature t and applied magnetic field h we find that sriro3 is a nonfermiliquid metal near a ferromagnetic instability as characterized by the following properties 1 small ordered moment but no evidence for longrange order down... | [['we', 'report', 'transport', 'and', 'thermodynamic', 'properties', 'of', 'singlecrystal', 'sriro3', 'as', 'a', 'function', 'of', 'temperature', 't', 'and', 'applied', 'magnetic', 'field', 'h', 'we', 'find', 'that', 'sriro3', 'is', 'a', 'nonfermiliquid', 'metal', 'near', 'a', 'ferromagnetic', 'instability', 'as', 'cha... | [-0.1994902280541802, 0.2740827941867922, -0.04343942716451628, 0.0017312799572079842, -0.022467298429858472, -0.18339520514210952, 0.14670899636486345, 0.3495775155723095, -0.24443332081594105, -0.30112852808088064, 0.0743202835421211, -0.33755866466755313, -0.09495062444226018, 0.18797261233848986, 0.0803669138046513... |
706.432 | Realization of Levy flights as continuous processes | On the basis of multivariate Langevin processes we present a realization of
Levy flights as a continuous process. For the simple case of a particle moving
under the influence of friction and a velocity dependent stochastic force we
explicitly derive the generalized Langevin equation and the corresponding
generalized ... | cond-mat.stat-mech cond-mat.mtrl-sci | on the basis of multivariate langevin processes we present a realization of levy flights as a continuous process for the simple case of a particle moving under the influence of friction and a velocity dependent stochastic force we explicitly derive the generalized langevin equation and the corresponding generalized fok... | [['on', 'the', 'basis', 'of', 'multivariate', 'langevin', 'processes', 'we', 'present', 'a', 'realization', 'of', 'levy', 'flights', 'as', 'a', 'continuous', 'process', 'for', 'the', 'simple', 'case', 'of', 'a', 'particle', 'moving', 'under', 'the', 'influence', 'of', 'friction', 'and', 'a', 'velocity', 'dependent', 's... | [-0.08650789580288086, 0.1295139604641937, -0.16739717347329444, 0.058727537574803985, -0.09230540336624897, -0.1278876778966886, 0.03442630913706764, 0.34264799962414705, -0.27929890345772135, -0.22923867492639322, 0.07304965379211972, -0.24041985163584034, -0.17765575351361979, 0.20946143405695267, -0.049421125968442... |
706.4321 | An optical surface resonance may render photonic crystals ineffective | In this work we identify and study the presence of extremely intense surface
resonances that frustrate the coupling of photons into a photonic crystal over
crucial energy ranges. The practical utility of photonic crystals demands the
capability to exchange photons with the external medium, therefore, it is
essential ... | cond-mat.mtrl-sci cond-mat.soft | in this work we identify and study the presence of extremely intense surface resonances that frustrate the coupling of photons into a photonic crystal over crucial energy ranges the practical utility of photonic crystals demands the capability to exchange photons with the external medium therefore it is essential to un... | [['in', 'this', 'work', 'we', 'identify', 'and', 'study', 'the', 'presence', 'of', 'extremely', 'intense', 'surface', 'resonances', 'that', 'frustrate', 'the', 'coupling', 'of', 'photons', 'into', 'a', 'photonic', 'crystal', 'over', 'crucial', 'energy', 'ranges', 'the', 'practical', 'utility', 'of', 'photonic', 'crysta... | [-0.13112700811276834, 0.1584090453469091, -0.061482069015295966, 0.01868213169509545, -0.10604660907346342, -0.12011713985767629, 0.0993069528007052, 0.43171069729659295, -0.27558668327724767, -0.34372367122107084, 0.03588864198342587, -0.27227573595527144, -0.14262881094020688, 0.17889945943477667, 0.0134179285003079... |
706.4322 | Measurement of the UHECR spectrum above 10 EeV at the Pierre Auger
Observatory using showers with zenith angles greater than 60 degrees | We report a measurement of the cosmic ray energy spectrum obtained using the
inclined events detected with the Pierre Auger Observatory. Showers with zenith
angles between 60 and 80 degrees recorded in the period between 1 January 2004
and 28 February 2007 are analysed. Showers are first reconstructed in arrival
dire... | astro-ph | we report a measurement of the cosmic ray energy spectrum obtained using the inclined events detected with the pierre auger observatory showers with zenith angles between 60 and 80 degrees recorded in the period between 1 january 2004 and 28 february 2007 are analysed showers are first reconstructed in arrival directio... | [['we', 'report', 'a', 'measurement', 'of', 'the', 'cosmic', 'ray', 'energy', 'spectrum', 'obtained', 'using', 'the', 'inclined', 'events', 'detected', 'with', 'the', 'pierre', 'auger', 'observatory', 'showers', 'with', 'zenith', 'angles', 'between', '60', 'and', '80', 'degrees', 'recorded', 'in', 'the', 'period', 'bet... | [-0.07023959794801089, 0.2086999104169298, -0.06555693138932893, 0.11253502897600254, 0.004072259294925563, -0.0025226102777888802, -0.029967009188927043, 0.44764625470140085, -0.2141087626683901, -0.4602816857175151, 0.009507090571543217, -0.3436699253854467, -0.014064400846055194, 0.18420329663568913, 0.0307031319434... |
706.4323 | Theory of Finite or Infinite Trees Revisited | We present in this paper a first-order axiomatization of an extended theory
$T$ of finite or infinite trees, built on a signature containing an infinite
set of function symbols and a relation $\fini(t)$ which enables to distinguish
between finite or infinite trees. We show that $T$ has at least one model and
prove it... | cs.LO cs.AI | we present in this paper a firstorder axiomatization of an extended theory t of finite or infinite trees built on a signature containing an infinite set of function symbols and a relation finit which enables to distinguish between finite or infinite trees we show that t has at least one model and prove its completeness... | [['we', 'present', 'in', 'this', 'paper', 'a', 'firstorder', 'axiomatization', 'of', 'an', 'extended', 'theory', 't', 'of', 'finite', 'or', 'infinite', 'trees', 'built', 'on', 'a', 'signature', 'containing', 'an', 'infinite', 'set', 'of', 'function', 'symbols', 'and', 'a', 'relation', 'finit', 'which', 'enables', 'to',... | [-0.12451077995392364, 0.06568403287835653, -0.11500915282265974, 0.08066406331466598, -0.11586706622725672, -0.18219655108218288, 0.1158125820374261, 0.346213238169029, -0.26386975728842754, -0.29112071115909616, 0.10744459050890888, -0.2466745177148769, -0.11374342315613142, 0.16262615310061973, -0.0413548399261024, ... |
706.4324 | Conformal coordinates of a constant density star | It is well known that the interior of a constant density spherical star is
conformally flat. In this paper we obtain the coordinate system in which the
conformal flatness of the metric manifests itself. In a similar way, we also
construct such coordinates for Robertson Walker metric.
| gr-qc | it is well known that the interior of a constant density spherical star is conformally flat in this paper we obtain the coordinate system in which the conformal flatness of the metric manifests itself in a similar way we also construct such coordinates for robertson walker metric | [['it', 'is', 'well', 'known', 'that', 'the', 'interior', 'of', 'a', 'constant', 'density', 'spherical', 'star', 'is', 'conformally', 'flat', 'in', 'this', 'paper', 'we', 'obtain', 'the', 'coordinate', 'system', 'in', 'which', 'the', 'conformal', 'flatness', 'of', 'the', 'metric', 'manifests', 'itself', 'in', 'a', 'sim... | [-0.1358740516403254, 0.07573231278938498, -0.12148724545903028, 0.0650121046705766, -0.10981937184771325, -0.10347725583755589, -0.06274711088762876, 0.3676630825279875, -0.23636932579919379, -0.2446536906534172, 0.08417712675377806, -0.23160054864599666, -0.21312247834941175, 0.10633552034801626, -0.12023291711205061... |
706.4325 | Disappearance of Squeezed Back-to-Back Correlations - a new signal of
hadron freeze-out from a supercooled Quark Gluon Plasma | We briefly discuss four different possible types of transitions from quark to
hadronic matter and their characteristic signatures in terms of correlations.
We also highlight the effects arising from mass modification of hadrons in hot
and dense hadronic matter, as well as their quantum statistical consequences:
the a... | nucl-th | we briefly discuss four different possible types of transitions from quark to hadronic matter and their characteristic signatures in terms of correlations we also highlight the effects arising from mass modification of hadrons in hot and dense hadronic matter as well as their quantum statistical consequences the appear... | [['we', 'briefly', 'discuss', 'four', 'different', 'possible', 'types', 'of', 'transitions', 'from', 'quark', 'to', 'hadronic', 'matter', 'and', 'their', 'characteristic', 'signatures', 'in', 'terms', 'of', 'correlations', 'we', 'also', 'highlight', 'the', 'effects', 'arising', 'from', 'mass', 'modification', 'of', 'ha... | [-0.10589771757672545, 0.2852007734141301, -0.15463908489946065, 0.14925694837429432, -0.01779994260095343, -0.10759532493087247, 0.02142471587481881, 0.32636780105334734, -0.23316572121254125, -0.29042755895714717, -0.01468185237230623, -0.3220173945367525, -0.03995808079162856, 0.1315385512796423, 0.0537278977373049,... |
706.4326 | The age grading and the Chen-Ruan cup product | We prove that the obstruction bundle used to define the cup-product in
Chen-Ruan cohomology is determined by the so-called `age grading' or
`degree-shifting numbers'. Indeed, the obstruction bundle can be directly
computed using the age grading. We obtain a Kunneth Theorem for Chen-Ruan
cohomology as a direct consequ... | math.AT math.AG | we prove that the obstruction bundle used to define the cupproduct in chenruan cohomology is determined by the socalled age grading or degreeshifting numbers indeed the obstruction bundle can be directly computed using the age grading we obtain a kunneth theorem for chenruan cohomology as a direct consequence of an ele... | [['we', 'prove', 'that', 'the', 'obstruction', 'bundle', 'used', 'to', 'define', 'the', 'cupproduct', 'in', 'chenruan', 'cohomology', 'is', 'determined', 'by', 'the', 'socalled', 'age', 'grading', 'or', 'degreeshifting', 'numbers', 'indeed', 'the', 'obstruction', 'bundle', 'can', 'be', 'directly', 'computed', 'using', ... | [-0.16539013702925798, 0.04631259914261849, -0.1503481895511819, 0.15392572936960622, -0.1318906240379186, -0.1267041545172499, -0.017358609280121083, 0.34254197695770777, -0.38101065027955416, -0.28987576591001973, 0.10997472974358478, -0.15534088992186496, -0.17644110682335482, 0.20818249634278282, -0.191195547165399... |
706.4327 | Dynamical structure factor at small q for the XXZ spin-1/2 chain | We combine Bethe Ansatz and field theory methods to study the longitudinal
dynamical structure factor S^{zz}(q,omega) for the anisotropic spin-1/2 chain
in the gapless regime. Using bosonization, we derive a low energy effective
model, including the leading irrelevant operators (band curvature terms) which
account fo... | cond-mat.str-el | we combine bethe ansatz and field theory methods to study the longitudinal dynamical structure factor szzqomega for the anisotropic spin12 chain in the gapless regime using bosonization we derive a low energy effective model including the leading irrelevant operators band curvature terms which account for boson decay p... | [['we', 'combine', 'bethe', 'ansatz', 'and', 'field', 'theory', 'methods', 'to', 'study', 'the', 'longitudinal', 'dynamical', 'structure', 'factor', 'szzqomega', 'for', 'the', 'anisotropic', 'spin12', 'chain', 'in', 'the', 'gapless', 'regime', 'using', 'bosonization', 'we', 'derive', 'a', 'low', 'energy', 'effective', ... | [-0.1306014106073778, 0.15768585574810706, -0.06373636233494004, 0.09888054799088168, -0.025790727677459057, -0.11413620046995104, 0.03477807172556956, 0.353774064870248, -0.2255695126039272, -0.2600930375110199, 0.04112673327263604, -0.2974504604971744, -0.07933504164377733, 0.14957137815641305, 0.10101252380664219, 0... |
706.4328 | QCD factorizations in gamma* gamma* --> rho_L^0 rho_L^0 | The exclusive reaction of rho meson pair electroproduction in gamma*gamma*
collisions is a nice place to study various dynamics and factorization
properties in the perturbative sector of QCD. At low energy (quarks dominance),
this process can be considered as a way to explore QCD factorizations involving
generalized ... | hep-ph | the exclusive reaction of rho meson pair electroproduction in gammagamma collisions is a nice place to study various dynamics and factorization properties in the perturbative sector of qcd at low energy quarks dominance this process can be considered as a way to explore qcd factorizations involving generalized distribu... | [['the', 'exclusive', 'reaction', 'of', 'rho', 'meson', 'pair', 'electroproduction', 'in', 'gammagamma', 'collisions', 'is', 'a', 'nice', 'place', 'to', 'study', 'various', 'dynamics', 'and', 'factorization', 'properties', 'in', 'the', 'perturbative', 'sector', 'of', 'qcd', 'at', 'low', 'energy', 'quarks', 'dominance',... | [-0.08476446397688198, 0.21455933164869403, -0.21986860425202123, 0.18763854933227964, -0.08488828800190454, -0.0998771392162247, 0.032073760373068264, 0.32714318347045745, -0.2380681905424458, -0.16485379330128774, -0.01798604402407447, -0.2952227253659532, -0.015469938642398894, 0.05342334699308521, 0.121544938818176... |
706.4329 | BF systems on graph cobordisms as topological cosmology | A cosmological model connecting the evolution of universe with a sequence of
topology changes described by a collection of specific graph cobordisms, is
constructed. It is shown that an adequate topological field theory (of BF-type)
can be put into relation to each graph cobordism. The explicit expressions for
transi... | gr-qc | a cosmological model connecting the evolution of universe with a sequence of topology changes described by a collection of specific graph cobordisms is constructed it is shown that an adequate topological field theory of bftype can be put into relation to each graph cobordism the explicit expressions for transition amp... | [['a', 'cosmological', 'model', 'connecting', 'the', 'evolution', 'of', 'universe', 'with', 'a', 'sequence', 'of', 'topology', 'changes', 'described', 'by', 'a', 'collection', 'of', 'specific', 'graph', 'cobordisms', 'is', 'constructed', 'it', 'is', 'shown', 'that', 'an', 'adequate', 'topological', 'field', 'theory', '... | [-0.20411205337489186, 0.13920215747099624, -0.08718080890381445, 0.10599343993382045, -0.08683433241438208, -0.12156960595120478, -0.00379905471757905, 0.31984815972409847, -0.2884025464465064, -0.2930996303857253, 0.03691791335678124, -0.26547077980523154, -0.18105198384986093, 0.12686193215030092, -0.023170633600863... |
706.433 | Molecular Outflows and a Mid-Infrared Census of the Massive
Star-Formation Region Associated with IRAS 18507+0121 | We have observed the central region of the IR-dark cloud filament associated
with IRAS 18507+0121 at millimeter wavelengths in CO(1-0), 13CO(1-0), and
C18O(1-0) line emission and with the Spitzer Space Telescope at mid-IR
wavelengths. Five massive outflows from two cloud cores were discovered. Three
outflows are cent... | astro-ph | we have observed the central region of the irdark cloud filament associated with iras 185070121 at millimeter wavelengths in co10 13co10 and c18o10 line emission and with the spitzer space telescope at midir wavelengths five massive outflows from two cloud cores were discovered three outflows are centered on or near an... | [['we', 'have', 'observed', 'the', 'central', 'region', 'of', 'the', 'irdark', 'cloud', 'filament', 'associated', 'with', 'iras', '185070121', 'at', 'millimeter', 'wavelengths', 'in', 'co10', '13co10', 'and', 'c18o10', 'line', 'emission', 'and', 'with', 'the', 'spitzer', 'space', 'telescope', 'at', 'midir', 'wavelength... | [-0.09334705067643274, 0.1126119181113049, -0.001246102221417599, 0.07352022841497141, -0.06747657892345968, -0.04192377053973321, 0.04103122277207211, 0.445550243018004, -0.12594532661346924, -0.34175802348181605, 0.08245850341597524, -0.27037986658083707, 0.00842487388021814, 0.15263337013858935, 0.015686808706835333... |
706.4331 | Constraints on Extrasolar Planet Populations from VLT NACO/SDI and MMT
SDI and Direct Adaptive Optics Imaging Surveys: Giant Planets are Rare at
Large Separations | We examine the implications for the distribution of extrasolar planets based
on the null results from two of the largest direct imaging surveys published to
date. Combining the measured contrast curves from 22 of the stars observed with
the VLT NACO adaptive optics system by Masciadri et al. (2005), and 48 of the
sta... | astro-ph | we examine the implications for the distribution of extrasolar planets based on the null results from two of the largest direct imaging surveys published to date combining the measured contrast curves from 22 of the stars observed with the vlt naco adaptive optics system by masciadri et al 2005 and 48 of the stars obse... | [['we', 'examine', 'the', 'implications', 'for', 'the', 'distribution', 'of', 'extrasolar', 'planets', 'based', 'on', 'the', 'null', 'results', 'from', 'two', 'of', 'the', 'largest', 'direct', 'imaging', 'surveys', 'published', 'to', 'date', 'combining', 'the', 'measured', 'contrast', 'curves', 'from', '22', 'of', 'the... | [-0.08629023156375183, 0.13907576897311513, -0.07288331894448956, 0.04364969197230624, -0.0904933059771776, -0.09498226562292751, 0.09620054772434135, 0.37645961143131956, -0.13401828450008385, -0.44823719906287457, 0.08267738121054036, -0.3033143528637445, -0.03165649821403627, 0.21317486048196171, -0.0421770412614782... |
706.4332 | Can 2HDM support fermion-stabilized bubbles of false vacuum? | The Higgs potential of the two-Higgs-doublet model can have several minima
with different properties. We discuss a possibility that a heavy fermion, if
trapped in a microscopic false vacuum bubble, might become light enough to
prevent the bubble from the collapse.
| hep-ph | the higgs potential of the twohiggsdoublet model can have several minima with different properties we discuss a possibility that a heavy fermion if trapped in a microscopic false vacuum bubble might become light enough to prevent the bubble from the collapse | [['the', 'higgs', 'potential', 'of', 'the', 'twohiggsdoublet', 'model', 'can', 'have', 'several', 'minima', 'with', 'different', 'properties', 'we', 'discuss', 'a', 'possibility', 'that', 'a', 'heavy', 'fermion', 'if', 'trapped', 'in', 'a', 'microscopic', 'false', 'vacuum', 'bubble', 'might', 'become', 'light', 'enough... | [-0.10437291189346735, 0.24149275500690792, -0.12925788274080288, 0.1471311851381892, -0.07704489514027245, -0.20031782216960337, 0.07064567608531655, 0.3239693432682898, -0.2179157168649864, -0.2555285680857373, 0.07641678202681516, -0.27994563491878716, -0.06959679384329696, 0.12931201835844394, -0.006303299425692275... |
706.4333 | Energy exchange in fast optical soliton collisions as a random cascade
model | We study the dynamics of a probe soliton propagating in an optical fiber and
exchanging energy in fast collisions with a random sequence of pump solitons.
The energy exchange is induced by Raman scattering or by cubic nonlinear
loss/gain. We show that the equation describing the dynamics of the probe
soliton's amplit... | nlin.PS | we study the dynamics of a probe soliton propagating in an optical fiber and exchanging energy in fast collisions with a random sequence of pump solitons the energy exchange is induced by raman scattering or by cubic nonlinear lossgain we show that the equation describing the dynamics of the probe solitons amplitude ha... | [['we', 'study', 'the', 'dynamics', 'of', 'a', 'probe', 'soliton', 'propagating', 'in', 'an', 'optical', 'fiber', 'and', 'exchanging', 'energy', 'in', 'fast', 'collisions', 'with', 'a', 'random', 'sequence', 'of', 'pump', 'solitons', 'the', 'energy', 'exchange', 'is', 'induced', 'by', 'raman', 'scattering', 'or', 'by',... | [-0.1757634435920395, 0.18753975312345, -0.1333516697623396, 0.09355922534806248, 0.02002240303392641, -0.08591972444472569, 0.0021296182732251858, 0.3387080127867009, -0.30166878090660204, -0.2407879348060018, 0.02619955634883836, -0.3034521282433455, -0.15877985932927272, 0.18890134993891575, 0.07601638094529062, 0.0... |
706.4334 | Power Loss for Inhomogeneous Poisson Processes | In this work, based on a realization of an inhomogeneous Poisson process
whose intensity function depends on a real unknown parameter, we consider a
simple hypothesis against a sequence of close (contiguous) alternatives. Under
certain regularity conditions we obtain the power loss of the score test with
respect to t... | math.ST stat.TH | in this work based on a realization of an inhomogeneous poisson process whose intensity function depends on a real unknown parameter we consider a simple hypothesis against a sequence of close contiguous alternatives under certain regularity conditions we obtain the power loss of the score test with respect to the neym... | [['in', 'this', 'work', 'based', 'on', 'a', 'realization', 'of', 'an', 'inhomogeneous', 'poisson', 'process', 'whose', 'intensity', 'function', 'depends', 'on', 'a', 'real', 'unknown', 'parameter', 'we', 'consider', 'a', 'simple', 'hypothesis', 'against', 'a', 'sequence', 'of', 'close', 'contiguous', 'alternatives', 'u... | [-0.1175776928566493, 0.020358726897998107, -0.09682848987883175, 0.0573845724357179, -0.06042578441163452, -0.09867445692153913, 0.08898914727841975, 0.3505212640776843, -0.23944418760645506, -0.26639132971902585, 0.11351202205035159, -0.21353500528380503, -0.14148972197980075, 0.1913196344363999, -0.09020935917611826... |
706.4335 | A single-photon transistor using nano-scale surface plasmons | It is well known that light quanta (photons) can interact with each other in
nonlinear media, much like massive particles do, but in practice these
interactions are usually very weak. Here we describe a novel approach to
realize strong nonlinear interactions at the single-photon level. Our method
makes use of recentl... | quant-ph | it is well known that light quanta photons can interact with each other in nonlinear media much like massive particles do but in practice these interactions are usually very weak here we describe a novel approach to realize strong nonlinear interactions at the singlephoton level our method makes use of recently demonst... | [['it', 'is', 'well', 'known', 'that', 'light', 'quanta', 'photons', 'can', 'interact', 'with', 'each', 'other', 'in', 'nonlinear', 'media', 'much', 'like', 'massive', 'particles', 'do', 'but', 'in', 'practice', 'these', 'interactions', 'are', 'usually', 'very', 'weak', 'here', 'we', 'describe', 'a', 'novel', 'approach... | [-0.14081594764518188, 0.23417937958278134, -0.051744675818000636, 0.04570259164893946, -0.09343438435082688, -0.21797630638963933, 0.034386996350224144, 0.47630524127811624, -0.2639529056023752, -0.31944933455046, 0.0022562795219119585, -0.28959942833466484, -0.15102339919278587, 0.21680461188046046, 0.009977702250488... |
706.4336 | On the Connection Between Metal Absorbers and Quasar Nebulae | We establish a simple model for the distribution of cold gas around L*
galaxies using a large set of observational constraints on the properties of
strong MgII absorber systems. Our analysis suggests that the halos of L*
galaxies are filled with cool gaseous clouds having sizes of order 1kpc and
densities of ~10^{-2}... | astro-ph | we establish a simple model for the distribution of cold gas around l galaxies using a large set of observational constraints on the properties of strong mgii absorber systems our analysis suggests that the halos of l galaxies are filled with cool gaseous clouds having sizes of order 1kpc and densities of 102 cm3 we th... | [['we', 'establish', 'a', 'simple', 'model', 'for', 'the', 'distribution', 'of', 'cold', 'gas', 'around', 'l', 'galaxies', 'using', 'a', 'large', 'set', 'of', 'observational', 'constraints', 'on', 'the', 'properties', 'of', 'strong', 'mgii', 'absorber', 'systems', 'our', 'analysis', 'suggests', 'that', 'the', 'halos', ... | [-0.0814118229965162, 0.08446620010662527, -0.04000773908725629, 0.09087124083501598, -0.06575009865272376, -0.07086397679781334, 0.016474105478523092, 0.42258228731031217, -0.11076951520517468, -0.32681704223569896, 0.03785260912975193, -0.30483173502660876, -0.012343019997287128, 0.19066726784221827, 0.01323309412433... |
706.4337 | Directed Paths in a Wedge | Directed paths have been used extensively in the scientific literature as a
model of a linear polymer. Such paths models in particular the conformational
entropy of a linear polymer and the effects it has on the free energy. These
directed models are simplified versions of the self-avoiding walk, but they do
neverthe... | cond-mat.soft cond-mat.stat-mech math-ph math.CO math.MP | directed paths have been used extensively in the scientific literature as a model of a linear polymer such paths models in particular the conformational entropy of a linear polymer and the effects it has on the free energy these directed models are simplified versions of the selfavoiding walk but they do nevertheless g... | [['directed', 'paths', 'have', 'been', 'used', 'extensively', 'in', 'the', 'scientific', 'literature', 'as', 'a', 'model', 'of', 'a', 'linear', 'polymer', 'such', 'paths', 'models', 'in', 'particular', 'the', 'conformational', 'entropy', 'of', 'a', 'linear', 'polymer', 'and', 'the', 'effects', 'it', 'has', 'on', 'the',... | [-0.12122659101372674, 0.15684833392821482, -0.09046784384304253, 0.027325933398161497, -0.052252253552001936, -0.1179969340018317, 0.017873452075821146, 0.3939143880196507, -0.2805490384202342, -0.23729670576494996, 0.07287303936019757, -0.2525249330312132, -0.18052918474447405, 0.13771956388175824, -0.042811695457973... |
706.4338 | Convergence properties of Donaldson's $T$-iterations on the Riemann
sphere | In a recent paper Donaldson defines three operators on a space of Hermitian
metrics on a complex projective manifold: $T, T_{\nu}, T_K.$ Iterations of
these operators converge to balanced metrics, and these themselves approximate
constant scalar curvature metrics. In this paper we investigate the convergence
properti... | math.DG math.NA | in a recent paper donaldson defines three operators on a space of hermitian metrics on a complex projective manifold t t_nu t_k iterations of these operators converge to balanced metrics and these themselves approximate constant scalar curvature metrics in this paper we investigate the convergence properties of these i... | [['in', 'a', 'recent', 'paper', 'donaldson', 'defines', 'three', 'operators', 'on', 'a', 'space', 'of', 'hermitian', 'metrics', 'on', 'a', 'complex', 'projective', 'manifold', 't', 't_nu', 't_k', 'iterations', 'of', 'these', 'operators', 'converge', 'to', 'balanced', 'metrics', 'and', 'these', 'themselves', 'approximat... | [-0.19664557724599802, 0.08916216628951212, -0.023022899611128703, 0.08899891802797183, -0.04761192182611142, -0.12027478011857186, 0.004968396554301892, 0.3502021422461858, -0.22706379171549565, -0.23621626156899664, 0.1273188845601879, -0.2891191193863513, -0.21876083026521853, 0.15930696843665035, -0.095128109449491... |
706.4339 | Dynamical and scaling properties of nu=5/2 interferometer | We calculate the non-linear I-V tunneling curves for a two-point-contact
tunneling junction between two edges of the $\nu={5/2}$ non-abelian fractional
quantum Hall state. The non-linear I-V tunneling curves are calculated for both
cases with and without an $e/4$ non-abelian quasiparticle between the two
contacts. We... | cond-mat.mes-hall cond-mat.str-el | we calculate the nonlinear iv tunneling curves for a twopointcontact tunneling junction between two edges of the nu52 nonabelian fractional quantum hall state the nonlinear iv tunneling curves are calculated for both cases with and without an e4 nonabelian quasiparticle between the two contacts we confirm that within a... | [['we', 'calculate', 'the', 'nonlinear', 'iv', 'tunneling', 'curves', 'for', 'a', 'twopointcontact', 'tunneling', 'junction', 'between', 'two', 'edges', 'of', 'the', 'nu52', 'nonabelian', 'fractional', 'quantum', 'hall', 'state', 'the', 'nonlinear', 'iv', 'tunneling', 'curves', 'are', 'calculated', 'for', 'both', 'case... | [-0.23143302857724213, 0.21699560717659255, -0.09921874696128936, 0.10155289147054604, -0.01324849340490737, -0.19460218924579623, 0.12023625311815332, 0.3566144282041594, -0.24479798186938603, -0.2756784650345528, -0.07649424884923149, -0.3636462553187685, -0.19109271951886111, 0.17182390799009523, 0.00366492298983990... |
706.434 | Analogue to multiple electromagnetically induced transparency in
all-optical drop-filter systems | We theoretically study a parallel optical configuration which includes N
periodically coupled whispering-gallery-mode resonators. The model shows an
obvious effect which has a direct analogy with the phenomenon of multiple
electromagnetically induced transparency in quantum systems. The numerical
simulations illumina... | quant-ph | we theoretically study a parallel optical configuration which includes n periodically coupled whisperinggallerymode resonators the model shows an obvious effect which has a direct analogy with the phenomenon of multiple electromagnetically induced transparency in quantum systems the numerical simulations illuminate tha... | [['we', 'theoretically', 'study', 'a', 'parallel', 'optical', 'configuration', 'which', 'includes', 'n', 'periodically', 'coupled', 'whisperinggallerymode', 'resonators', 'the', 'model', 'shows', 'an', 'obvious', 'effect', 'which', 'has', 'a', 'direct', 'analogy', 'with', 'the', 'phenomenon', 'of', 'multiple', 'electro... | [-0.21546115275294356, 0.15406667721403852, -0.04540644584716681, 0.004496324506095227, -0.031414731213932526, -0.16621759105199838, 0.03619623622473549, 0.4834167289081961, -0.24816993664374903, -0.2518665098639972, 0.049058097630383116, -0.2688150370411356, -0.19077718140461536, 0.25358653106548656, -0.00121110225068... |
706.4341 | A note on p-adic q-integrals associated with q-Euler numbers | In this we give a detailed proof of fermionic p-adic q-measures on Z_p and we
will treat some interesting formulae related q-extension of Euler numbers and
polynomials.
| math.NT | in this we give a detailed proof of fermionic padic qmeasures on z_p and we will treat some interesting formulae related qextension of euler numbers and polynomials | [['in', 'this', 'we', 'give', 'a', 'detailed', 'proof', 'of', 'fermionic', 'padic', 'qmeasures', 'on', 'z_p', 'and', 'we', 'will', 'treat', 'some', 'interesting', 'formulae', 'related', 'qextension', 'of', 'euler', 'numbers', 'and', 'polynomials']] | [-0.2543510030417775, 0.10374826669850826, -0.1849559676976731, 0.16946141417765131, -0.15519515224374258, -0.13568168045737997, 0.024959285779354665, 0.24949920725507232, -0.2349908945079033, -0.21573762044024009, 0.05409991903714119, -0.22727363921092966, -0.18704458318937284, 0.2813924238658868, -0.13801670995039436... |
706.4342 | Spin-liquid model of the sharp resistivity drop in
$La_{1.85}Ba_{0.125}CuO_4$ | We use the phenomenological model proposed in our previous paper [Phys. Rev.
Lett. {\bf 98}, 237001 (2007)] to analyse the magnetic field dependence of the
onset temperature for two-dimensional fluctuating superconductivity $T^{**}
(H)$. We demonstrate that the slope of $T^{**} (H)$ progressively goes down as
$H$ inc... | cond-mat.supr-con | we use the phenomenological model proposed in our previous paper phys rev lett bf 98 237001 2007 to analyse the magnetic field dependence of the onset temperature for twodimensional fluctuating superconductivity t h we demonstrate that the slope of t h progressively goes down as h increases such that the upper critical... | [['we', 'use', 'the', 'phenomenological', 'model', 'proposed', 'in', 'our', 'previous', 'paper', 'phys', 'rev', 'lett', 'bf', '98', '237001', '2007', 'to', 'analyse', 'the', 'magnetic', 'field', 'dependence', 'of', 'the', 'onset', 'temperature', 'for', 'twodimensional', 'fluctuating', 'superconductivity', 't', 'h', 'we... | [-0.08795531174925329, 0.16526483345756326, -0.005405230058746023, -0.05396739102178509, -0.03861884838277167, -0.07448682863429025, 0.1013318600432415, 0.3218367665105469, -0.1844511013682727, -0.3676818992410387, -0.013688101210621195, -0.3099385329245866, -0.09736850565033299, 0.1827860228220963, -0.0393151026782016... |
706.4343 | Hausdorff Dimension and Hausdorff Measure for Non-integer based
Cantor-type Sets | We consider digits-deleted sets or Cantor-type sets with $\beta$-expansions.
We calculate the Hausdorff dimension $d$ of these sets and show that $d$ is
continuous with respect to $\beta$. The $d$-dimentional Hausdorff measure of
these sets is finite and positive.
| math.DS math.MG | we consider digitsdeleted sets or cantortype sets with betaexpansions we calculate the hausdorff dimension d of these sets and show that d is continuous with respect to beta the ddimentional hausdorff measure of these sets is finite and positive | [['we', 'consider', 'digitsdeleted', 'sets', 'or', 'cantortype', 'sets', 'with', 'betaexpansions', 'we', 'calculate', 'the', 'hausdorff', 'dimension', 'd', 'of', 'these', 'sets', 'and', 'show', 'that', 'd', 'is', 'continuous', 'with', 'respect', 'to', 'beta', 'the', 'ddimentional', 'hausdorff', 'measure', 'of', 'these'... | [-0.14483022063064413, 0.1701222560242624, -0.02885397456938753, 0.09342630291231782, 0.03607301148460121, -0.11960242593006508, 0.05657046197636707, 0.38425752510492867, -0.3026801720261574, -0.13524473070425005, 0.09790093575075672, -0.3985573804459056, -0.08787565354282993, 0.189484607119969, -0.08076654052412188, 0... |
706.4344 | 2-Selmer Groups and the Birch-Swinnerton-Dyer Conjecture for the
Congruent Number Curve | We take an approach toward counting the number of n for which the curves E_n:
y^2=x^3-n^2x have 2-Selmer groups of a given size. This question was also
discussed in a pair of Invent. Math. papers by Roger Heath-Brown. We discuss
the connection between computing the size of these Selmer groups and verifying
cases of t... | math.NT | we take an approach toward counting the number of n for which the curves e_n y2x3n2x have 2selmer groups of a given size this question was also discussed in a pair of invent math papers by roger heathbrown we discuss the connection between computing the size of these selmer groups and verifying cases of the birch and s... | [['we', 'take', 'an', 'approach', 'toward', 'counting', 'the', 'number', 'of', 'n', 'for', 'which', 'the', 'curves', 'e_n', 'y2x3n2x', 'have', '2selmer', 'groups', 'of', 'a', 'given', 'size', 'this', 'question', 'was', 'also', 'discussed', 'in', 'a', 'pair', 'of', 'invent', 'math', 'papers', 'by', 'roger', 'heathbrown'... | [-0.20063563762774128, 0.06257146108987928, -0.12279565877627668, 0.07548916160648819, -0.039790310114513824, -0.12447865301916419, 0.03502159132040106, 0.257740703303107, -0.2463142105194112, -0.34123275994301533, 0.03341069210288223, -0.2615323765365797, -0.12121003171764748, 0.2198690879916729, -0.10863204952329397,... |
706.4345 | NMR relaxation and resistivity from rattling phonons in pyrochlore
superconductors | We calculate the temperature dependence of NMR relaxation rate and electrical
resistivity for coupling to a local, strongly anharmonic phonon mode. We argue
that the two-phonon Raman process is dominating NMR relaxation. Due to the
strong anharmonicity of the phonon an unusual temperature dependence is found
having a... | cond-mat.supr-con cond-mat.mtrl-sci | we calculate the temperature dependence of nmr relaxation rate and electrical resistivity for coupling to a local strongly anharmonic phonon mode we argue that the twophonon raman process is dominating nmr relaxation due to the strong anharmonicity of the phonon an unusual temperature dependence is found having a low t... | [['we', 'calculate', 'the', 'temperature', 'dependence', 'of', 'nmr', 'relaxation', 'rate', 'and', 'electrical', 'resistivity', 'for', 'coupling', 'to', 'a', 'local', 'strongly', 'anharmonic', 'phonon', 'mode', 'we', 'argue', 'that', 'the', 'twophonon', 'raman', 'process', 'is', 'dominating', 'nmr', 'relaxation', 'due'... | [-0.14452140476140712, 0.24842694652244163, -0.05279249058415492, -0.006776795503194282, -0.06236885783469511, -0.18364354581572115, 0.08362237218146523, 0.4098844524886873, -0.24194603173269166, -0.2457037020371192, 0.017268549085646453, -0.375162194793423, -0.06411049475686417, 0.23025972979764145, 0.0542479530811760... |
706.4346 | Studying possible CP-violating Higgs couplings through top-quark pair
productions at muon colliders | We study possible anomalous CP-violating Higgs couplings to mu mu-bar and t
t-bar fully model-independent way through top-quark pair productions at muon
colliders. Assuming additional non-standard neutral Higgs bosons, whose
couplings with top-quark and muon are expressed in the most general covariant
form, we carry ... | hep-ph hep-ex | we study possible anomalous cpviolating higgs couplings to mu mubar and t tbar fully modelindependent way through topquark pair productions at muon colliders assuming additional nonstandard neutral higgs bosons whose couplings with topquark and muon are expressed in the most general covariant form we carry out analyses... | [['we', 'study', 'possible', 'anomalous', 'cpviolating', 'higgs', 'couplings', 'to', 'mu', 'mubar', 'and', 't', 'tbar', 'fully', 'modelindependent', 'way', 'through', 'topquark', 'pair', 'productions', 'at', 'muon', 'colliders', 'assuming', 'additional', 'nonstandard', 'neutral', 'higgs', 'bosons', 'whose', 'couplings'... | [-0.09950144076350308, 0.259235222614301, -0.05119191100248062, 0.13664435415384582, -0.1283177515022486, -0.192148875116208, 0.038967574951201976, 0.3478190889434209, -0.24155000058863874, -0.27771815518656423, 0.030723985863871695, -0.31044921676983084, -0.021699262442924673, 0.1723646939776483, 0.0751321036590352, 0... |
706.4347 | Bulge and Halo Kinematics Across the Hubble Sequence | The correlation between the maximum rotational velocity of the disk (v_m) and
the central stellar velocity dispersion of the bulge (sigma) offers insights
into the relationship between the halo and the bulge. We have assembled
integrated H I line widths and central stellar velocity dispersions to study
the v_m-sigma ... | astro-ph | the correlation between the maximum rotational velocity of the disk v_m and the central stellar velocity dispersion of the bulge sigma offers insights into the relationship between the halo and the bulge we have assembled integrated h i line widths and central stellar velocity dispersions to study the v_msigma relation... | [['the', 'correlation', 'between', 'the', 'maximum', 'rotational', 'velocity', 'of', 'the', 'disk', 'v_m', 'and', 'the', 'central', 'stellar', 'velocity', 'dispersion', 'of', 'the', 'bulge', 'sigma', 'offers', 'insights', 'into', 'the', 'relationship', 'between', 'the', 'halo', 'and', 'the', 'bulge', 'we', 'have', 'ass... | [-0.07330795621471355, 0.09572061843521494, -0.13267116636234277, 0.10607202073827336, -0.11890586227881224, -0.06304885779068822, 0.04202432467510724, 0.41714091149125515, -0.1669495920692238, -0.3518399137932907, 0.009999347064876929, -0.2847502139671373, -0.04583812309387473, 0.18515492494704436, 0.00369145179813910... |
706.4348 | A fast direct solver for network matrices | A fast direct inversion scheme for the large sparse systems of linear
equations resulting from the discretization of elliptic partial differential
equations in two dimensions is given. The scheme is described for the
particular case of a discretization on a uniform square grid, but can be
generalized to more general ... | math.NA | a fast direct inversion scheme for the large sparse systems of linear equations resulting from the discretization of elliptic partial differential equations in two dimensions is given the scheme is described for the particular case of a discretization on a uniform square grid but can be generalized to more general geom... | [['a', 'fast', 'direct', 'inversion', 'scheme', 'for', 'the', 'large', 'sparse', 'systems', 'of', 'linear', 'equations', 'resulting', 'from', 'the', 'discretization', 'of', 'elliptic', 'partial', 'differential', 'equations', 'in', 'two', 'dimensions', 'is', 'given', 'the', 'scheme', 'is', 'described', 'for', 'the', 'pa... | [-0.15613007849416413, 0.06955197920267339, -0.006907763371271068, 0.04521563461394575, -0.04219271695794727, -0.18658496141501202, 0.05050841468197388, 0.3382780225272628, -0.262255418991697, -0.3137013386020545, 0.1609451308301515, -0.28664988306674943, -0.07715273216414009, 0.2450027752438209, -0.05390271071034173, ... |
706.4349 | TeV scale partial mirage unification and neutralino dark matter | We study the TeV scale partial mirage unification scenario, where the gluino
and wino masses are degenerate around a TeV scale, but the bino mass is not
degenerate. This scenario has phenomenologically interesting aspects. First,
because of the degeneracy between the gluino and wino masses, this scenario
does not hav... | hep-ph | we study the tev scale partial mirage unification scenario where the gluino and wino masses are degenerate around a tev scale but the bino mass is not degenerate this scenario has phenomenologically interesting aspects first because of the degeneracy between the gluino and wino masses this scenario does not have the li... | [['we', 'study', 'the', 'tev', 'scale', 'partial', 'mirage', 'unification', 'scenario', 'where', 'the', 'gluino', 'and', 'wino', 'masses', 'are', 'degenerate', 'around', 'a', 'tev', 'scale', 'but', 'the', 'bino', 'mass', 'is', 'not', 'degenerate', 'this', 'scenario', 'has', 'phenomenologically', 'interesting', 'aspects... | [-0.12073477183231886, 0.2855370903565559, -0.051375854336604306, 0.22689866961314856, -0.13122716872021556, -0.17108004042627603, 0.025098122096505394, 0.3305097524458647, -0.20294698743212425, -0.39242579762855273, 0.08540454883588834, -0.24643484369087754, 0.0518814589660824, 0.11526539697301354, 0.00378042349612779... |
706.435 | On Interdependence of the Paleomagnetic Field Characteristics | The behaviour of the geomagnetic field characteristics (mean values of the
paleointensity, amplitude of its variations and reversal frequency) during the
last 170 million years was analyzed. It was found that the mean values of the
paleointensity were in direct relation to amplitude of its variations and in
reverse r... | physics.geo-ph | the behaviour of the geomagnetic field characteristics mean values of the paleointensity amplitude of its variations and reversal frequency during the last 170 million years was analyzed it was found that the mean values of the paleointensity were in direct relation to amplitude of its variations and in reverse relatio... | [['the', 'behaviour', 'of', 'the', 'geomagnetic', 'field', 'characteristics', 'mean', 'values', 'of', 'the', 'paleointensity', 'amplitude', 'of', 'its', 'variations', 'and', 'reversal', 'frequency', 'during', 'the', 'last', '170', 'million', 'years', 'was', 'analyzed', 'it', 'was', 'found', 'that', 'the', 'mean', 'valu... | [-0.16469860269377629, 0.17930045566253183, -0.1108029412623081, 0.07241621119901538, -0.04665684923529625, 0.004976278310641647, 0.018482083382291927, 0.3746354890780316, -0.24209644202168823, -0.37367114608900415, 0.1018032297401482, -0.24574583247303963, -0.13669905356234974, 0.20769346680543904, -0.0574780683033168... |
706.4351 | Diffuse Gamma-ray Emission from the Galactic Center - A Multiple Energy
Injection Model | We suggest that the energy source of the observed diffuse gamma-ray emission
from the direction of the Galactic center is the Galactic black hole Sgr A*,
which becomes active when a star is captured at a rate of $\sim 10^{-5} $
yr^{-1}. Subsequently the star is tidally disrupted and its matter is accreted
into the bl... | astro-ph | we suggest that the energy source of the observed diffuse gammaray emission from the direction of the galactic center is the galactic black hole sgr a which becomes active when a star is captured at a rate of sim 105 yr1 subsequently the star is tidally disrupted and its matter is accreted into the black hole during th... | [['we', 'suggest', 'that', 'the', 'energy', 'source', 'of', 'the', 'observed', 'diffuse', 'gammaray', 'emission', 'from', 'the', 'direction', 'of', 'the', 'galactic', 'center', 'is', 'the', 'galactic', 'black', 'hole', 'sgr', 'a', 'which', 'becomes', 'active', 'when', 'a', 'star', 'is', 'captured', 'at', 'a', 'rate', '... | [-0.038450781369573195, 0.23266763456976386, -0.03611517593057619, 0.13172413551472817, -0.018264920549053286, -0.05556628629047838, 0.030619496810767387, 0.3724631965039643, -0.19856796977282673, -0.3630205032536415, -0.017914817900897037, -0.34896554945519676, 0.11037479464602828, 0.19757423608529348, 0.0167170206817... |
706.4352 | Orbital Order, Stripe Phases and Mott Transition in a Planar Model for
Manganites | Understanding orbital ordered (OO) Mott insulating states lies at the heart
of a consistent resolution of the colossal magneto-resistance (CMR) observed in
manganites, where its melting induces a low-$T$ insulator-metal transition for
$0.25 \le x\le 0.45$. Motivated thereby, we study the OO states in a planar
model f... | cond-mat.str-el cond-mat.mtrl-sci | understanding orbital ordered oo mott insulating states lies at the heart of a consistent resolution of the colossal magnetoresistance cmr observed in manganites where its melting induces a lowt insulatormetal transition for 025 le xle 045 motivated thereby we study the oo states in a planar model for bilayer manganite... | [['understanding', 'orbital', 'ordered', 'oo', 'mott', 'insulating', 'states', 'lies', 'at', 'the', 'heart', 'of', 'a', 'consistent', 'resolution', 'of', 'the', 'colossal', 'magnetoresistance', 'cmr', 'observed', 'in', 'manganites', 'where', 'its', 'melting', 'induces', 'a', 'lowt', 'insulatormetal', 'transition', 'for... | [-0.17262991683441214, 0.18976632181220338, -0.012081389497034252, 0.08525510977022349, 0.022539968849159778, -0.1687684104568325, 0.12210174044128508, 0.4007776490226388, -0.25153774266829715, -0.24307945475913584, 0.0023004741175100206, -0.3693691019853577, -0.1152765273116529, 0.12275670675560832, 0.0412753589916974... |
706.4353 | Geometric Invariant Theory via Cox Rings | We consider actions of reductive groups on a varieties with finitely
generated Cox ring, e.g., the classical case of a diagonal action on a product
of projective spaces. Given such an action, we construct via combinatorial data
in the Cox ring all maximal open subsets such that the quotient is
quasiprojective or embe... | math.AG | we consider actions of reductive groups on a varieties with finitely generated cox ring eg the classical case of a diagonal action on a product of projective spaces given such an action we construct via combinatorial data in the cox ring all maximal open subsets such that the quotient is quasiprojective or embeddable i... | [['we', 'consider', 'actions', 'of', 'reductive', 'groups', 'on', 'a', 'varieties', 'with', 'finitely', 'generated', 'cox', 'ring', 'eg', 'the', 'classical', 'case', 'of', 'a', 'diagonal', 'action', 'on', 'a', 'product', 'of', 'projective', 'spaces', 'given', 'such', 'an', 'action', 'we', 'construct', 'via', 'combinato... | [-0.17726085986037857, -0.001286058222990284, -0.08898304482397523, 0.049221150098974334, -0.11167741000417222, -0.10519113576093923, -0.03161168943478011, 0.3567124935572298, -0.36081582872486373, -0.158377395997059, 0.15035955144490287, -0.24280313745104862, -0.1364464227480868, 0.2600383054333947, -0.174208250683415... |
706.4354 | A counterexample to generalizations of the Milnor-Bloch-Kato conjecture | We construct an example of a torus $T$ over a field $K$ for which the Galois
symbol $K(K; T,T)/n K(K; T,T) \to H^2(K, T[n]\otimes T[n])$ is not injective
for some $n$. Here $K(K; T,T)$ is the Milnor $K$-group attached to $T$
introduced by Somekawa. We show also that the motive $M(T\times T)$ gives a
counterexample to... | math.KT | we construct an example of a torus t over a field k for which the galois symbol kk ttn kk tt to h2k tnotimes tn is not injective for some n here kk tt is the milnor kgroup attached to t introduced by somekawa we show also that the motive mttimes t gives a counterexample to another generalization of the milnorblochkato ... | [['we', 'construct', 'an', 'example', 'of', 'a', 'torus', 't', 'over', 'a', 'field', 'k', 'for', 'which', 'the', 'galois', 'symbol', 'kk', 'ttn', 'kk', 'tt', 'to', 'h2k', 'tnotimes', 'tn', 'is', 'not', 'injective', 'for', 'some', 'n', 'here', 'kk', 'tt', 'is', 'the', 'milnor', 'kgroup', 'attached', 'to', 't', 'introduc... | [-0.21456519780199854, 0.11711598771474993, -0.1365358990827395, 0.05272254389485404, -0.1117555475343139, -0.2050628560039425, 0.020049265255370447, 0.2714701004086002, -0.33796165769378983, -0.2016765424651244, 0.02496200275697535, -0.2398165440470386, -0.14756628773325392, 0.19566709557247738, -0.11362373418054514, ... |
706.4355 | Phase Space Constraints on Neutrino Luminosities | While the importance of phase space constraints for gravitational clustering
of neutrinos (which are fermions) is well recognized, the explicit use of such
constraints to limit neutrino emission from ultra energetic sources has not
been stressed. Special and general relativistic phase space constraints are
shown to l... | astro-ph | while the importance of phase space constraints for gravitational clustering of neutrinos which are fermions is well recognized the explicit use of such constraints to limit neutrino emission from ultra energetic sources has not been stressed special and general relativistic phase space constraints are shown to limit n... | [['while', 'the', 'importance', 'of', 'phase', 'space', 'constraints', 'for', 'gravitational', 'clustering', 'of', 'neutrinos', 'which', 'are', 'fermions', 'is', 'well', 'recognized', 'the', 'explicit', 'use', 'of', 'such', 'constraints', 'to', 'limit', 'neutrino', 'emission', 'from', 'ultra', 'energetic', 'sources', '... | [-0.08557636144952002, 0.2064440062946894, -0.04596152816983787, 0.2057115661932833, -0.1263465488498861, -0.07587259012189779, 0.015119777924635194, 0.4020295051688498, -0.1865260019221089, -0.3203079810874029, 0.09348405781202018, -0.2937231665434824, -0.041852780490775, 0.23549064787274057, 0.007957833649759943, 0.0... |
706.4356 | A three-dimensional backward-wave network matched with free space | A backward-wave slab based on a capacitively and inductively loaded
three-dimensional transmission-line network is designed in such a way that
impedance-matching with free space is obtained. To enable field propagation
from free space to the network and vice versa, the use of a transition layer is
proposed. Matching ... | physics.gen-ph physics.optics | a backwardwave slab based on a capacitively and inductively loaded threedimensional transmissionline network is designed in such a way that impedancematching with free space is obtained to enable field propagation from free space to the network and vice versa the use of a transition layer is proposed matching of the de... | [['a', 'backwardwave', 'slab', 'based', 'on', 'a', 'capacitively', 'and', 'inductively', 'loaded', 'threedimensional', 'transmissionline', 'network', 'is', 'designed', 'in', 'such', 'a', 'way', 'that', 'impedancematching', 'with', 'free', 'space', 'is', 'obtained', 'to', 'enable', 'field', 'propagation', 'from', 'free'... | [-0.10462792456725284, 0.1395798865979647, -0.023306470179437277, -0.04581682882716825, -0.1146136972341029, -0.17643866482231876, 0.034608780481743026, 0.4734010218697436, -0.22363889513208585, -0.2788253708961694, 0.07652022683588952, -0.2747744657784043, -0.16442267532350824, 0.19179708761272624, 0.01632810894208138... |
706.4357 | Nuclear deformation and the two neutrino double-\beta decay in
^{124,126}Xe,^{128,130}Te, ^{130,132}Ba and ^{150}Nd isotopes | The two neutrino double beta decay of $^{124,126}$Xe,$^{128,130}$Te, $
^{130,132}$Ba and $^{150}$Nd isotopes is studied in the Projected
Hartree-Fock-Bogoliubov (PHFB) model. Theoretical 2$\nu $ $\beta^{-}\beta ^{-}$
half-lives of $^{128,130}$Te, and $^{150}$Nd isotopes, and 2$\nu
\beta^{+}\beta^{+}$, 2$\nu $ $\beta^... | nucl-th | the two neutrino double beta decay of 124126xe128130te 130132ba and 150nd isotopes is studied in the projected hartreefockbogoliubov phfb model theoretical 2nu betabeta halflives of 128130te and 150nd isotopes and 2nu betabeta 2nu betaec and 2nu ecec for 124126xe and 130132ba nuclei are presented calculated quadrupolar... | [['the', 'two', 'neutrino', 'double', 'beta', 'decay', 'of', '124126xe128130te', '130132ba', 'and', '150nd', 'isotopes', 'is', 'studied', 'in', 'the', 'projected', 'hartreefockbogoliubov', 'phfb', 'model', 'theoretical', '2nu', 'betabeta', 'halflives', 'of', '128130te', 'and', '150nd', 'isotopes', 'and', '2nu', 'betabe... | [-0.009542834083282057, 0.2724473564189741, 0.04577746017482774, 0.1879662885625001, 0.10254312533585505, -0.16506296320251007, 0.08748553622642467, 0.3456937124117695, -0.1451726035247075, -0.18405537617435658, -0.04685765904931073, -0.36286260431696626, -0.0048984846354618765, 0.128092083657139, 0.14572308046593405, ... |
706.4358 | On Wahl's proof of $\mu(6)=65$ | D. Jaffe and D. Ruberman proved in 1997 that a sextic hypersurface in
$\mathbb{P}^3$ has at most 65 nodes (the bound is sharp by Barth's
construction).
Almost at the same time, J. Wahl proposed a much shorter proof of the same
result, by proving that a linear code $V\subset \F^{66}$ with weights in
$\{24,32,40\}$ h... | math.AG | d jaffe and d ruberman proved in 1997 that a sextic hypersurface in mathbbp3 has at most 65 nodes the bound is sharp by barths construction almost at the same time j wahl proposed a much shorter proof of the same result by proving that a linear code vsubset f66 with weights in 243240 has dimension dimvleq12 he claimed ... | [['d', 'jaffe', 'and', 'd', 'ruberman', 'proved', 'in', '1997', 'that', 'a', 'sextic', 'hypersurface', 'in', 'mathbbp3', 'has', 'at', 'most', '65', 'nodes', 'the', 'bound', 'is', 'sharp', 'by', 'barths', 'construction', 'almost', 'at', 'the', 'same', 'time', 'j', 'wahl', 'proposed', 'a', 'much', 'shorter', 'proof', 'of... | [-0.1310750707395046, 0.08495429286712726, -0.06245872488738421, 0.04204120321185602, -0.027486595484044623, -0.19162160455769695, 0.07179743595256963, 0.2812786752933308, -0.2255158453611383, -0.3100024674361681, 0.07704376643181175, -0.2847232882399112, -0.12315311715424554, 0.1920635015128509, -0.1286146507728571, 0... |
706.4359 | Existence of positive representations for complex weights | The necessity of computing integrals with complex weights over manifolds with
a large number of dimensions, e.g., in some field theoretical settings, poses a
problem for the use of Monte Carlo techniques. Here it is shown that very
general complex weight functions P(x) on R^d can be represented by real and
positive w... | hep-lat math-ph math.MP | the necessity of computing integrals with complex weights over manifolds with a large number of dimensions eg in some field theoretical settings poses a problem for the use of monte carlo techniques here it is shown that very general complex weight functions px on rd can be represented by real and positive weights pz o... | [['the', 'necessity', 'of', 'computing', 'integrals', 'with', 'complex', 'weights', 'over', 'manifolds', 'with', 'a', 'large', 'number', 'of', 'dimensions', 'eg', 'in', 'some', 'field', 'theoretical', 'settings', 'poses', 'a', 'problem', 'for', 'the', 'use', 'of', 'monte', 'carlo', 'techniques', 'here', 'it', 'is', 'sh... | [-0.13405391972736214, 0.06738036507625639, -0.05183412228929408, 0.06788154200788725, -0.08205320889613142, -0.13301907776406519, 0.002304654367222094, 0.396234137730466, -0.27009225602227227, -0.2413067190712433, 0.11044340570066354, -0.23112333662531995, -0.17469506029235085, 0.24687114369446111, -0.0505945414597927... |
706.436 | Cold r-Process in Neutrino-Driven Winds | The r-process in a low temperature environment is explored, in which the
neutron emission by photodisintegration does not play a role (cold r-process).
A semi-analytic neutrino-driven wind model is utilized for this purpose. The
temperature in a supersonically expanding outflow can quickly drop to a few
10^8 K, where... | astro-ph | the rprocess in a low temperature environment is explored in which the neutron emission by photodisintegration does not play a role cold rprocess a semianalytic neutrinodriven wind model is utilized for this purpose the temperature in a supersonically expanding outflow can quickly drop to a few 108 k where the n gammag... | [['the', 'rprocess', 'in', 'a', 'low', 'temperature', 'environment', 'is', 'explored', 'in', 'which', 'the', 'neutron', 'emission', 'by', 'photodisintegration', 'does', 'not', 'play', 'a', 'role', 'cold', 'rprocess', 'a', 'semianalytic', 'neutrinodriven', 'wind', 'model', 'is', 'utilized', 'for', 'this', 'purpose', 'th... | [-0.043421072079306185, 0.22125144590708343, -0.07323566015640443, 0.13745750348475252, -0.04164378755376674, -0.09645264120208043, 0.04310188496090246, 0.3524247489756707, -0.21082113019303617, -0.3151482746541274, -0.01599244318133446, -0.27578821857318736, 0.033998703763989564, 0.19523841410762433, -0.02129223118324... |
706.4361 | J/psi production in Indium-Indium collisions at 158 GeV/nucleon | The NA60 experiment studies muon pair production at the CERN SPS. In this
letter we report on a precision measurement of J/psi in In-In collisions. We
have studied the J/psi centrality distribution, and we have compared it with
the one expected if absorption in cold nuclear matter were the only active
suppression mec... | nucl-ex | the na60 experiment studies muon pair production at the cern sps in this letter we report on a precision measurement of jpsi in inin collisions we have studied the jpsi centrality distribution and we have compared it with the one expected if absorption in cold nuclear matter were the only active suppression mechanism f... | [['the', 'na60', 'experiment', 'studies', 'muon', 'pair', 'production', 'at', 'the', 'cern', 'sps', 'in', 'this', 'letter', 'we', 'report', 'on', 'a', 'precision', 'measurement', 'of', 'jpsi', 'in', 'inin', 'collisions', 'we', 'have', 'studied', 'the', 'jpsi', 'centrality', 'distribution', 'and', 'we', 'have', 'compare... | [-0.062418390799460835, 0.19867599901734043, -0.1623830252130957, 0.11306121495037683, -0.006748152340419198, -0.10759949209168554, -0.021739327076724484, 0.38755669423231953, -0.13405180216619844, -0.33514422850781367, -0.05999856607400273, -0.4187935568392277, 0.011113980716388477, 0.1608700177779323, 0.0322930402073... |
706.4362 | A Special Nonlinear Connection in Second Order Geometry | We show that, for mechanical system with external forces, the equations of
deviations of solution curves of the corresponding Lagrange equations,determine
a nonlinear connection on the second order osculator (second order tangent)
bundle. In particular, Jacobi equations in Finsler and Riemann spaces determine
such a ... | math.DG math-ph math.MP | we show that for mechanical system with external forces the equations of deviations of solution curves of the corresponding lagrange equationsdetermine a nonlinear connection on the second order osculator second order tangent bundle in particular jacobi equations in finsler and riemann spaces determine such a nonlinear... | [['we', 'show', 'that', 'for', 'mechanical', 'system', 'with', 'external', 'forces', 'the', 'equations', 'of', 'deviations', 'of', 'solution', 'curves', 'of', 'the', 'corresponding', 'lagrange', 'equationsdetermine', 'a', 'nonlinear', 'connection', 'on', 'the', 'second', 'order', 'osculator', 'second', 'order', 'tangen... | [-0.2229462358088273, 0.02638919490298418, -0.06608761689099281, 0.07491718382453141, -0.1427320109822018, -0.09258872865820708, -0.038806203469310116, 0.29561949322890974, -0.3173557369281416, -0.23429850209504366, 0.09613352688535562, -0.283369036472362, -0.2378619754605967, 0.1744529819520919, -0.05031562056999816, ... |
706.4363 | Vacuum polarization and plasma oscillations | We evidence the existence of plasma oscillations of electrons-positron pairs
created by the vacuum polarization in an uniform electric field with E < Ec.
Our general treatment, encompassing also the traditional, well studied case of
E > Ec, shows the existence in both cases of a maximum Lorentz factor acquired
by ele... | astro-ph physics.plasm-ph | we evidence the existence of plasma oscillations of electronspositron pairs created by the vacuum polarization in an uniform electric field with e ec our general treatment encompassing also the traditional well studied case of e ec shows the existence in both cases of a maximum lorentz factor acquired by electrons and ... | [['we', 'evidence', 'the', 'existence', 'of', 'plasma', 'oscillations', 'of', 'electronspositron', 'pairs', 'created', 'by', 'the', 'vacuum', 'polarization', 'in', 'an', 'uniform', 'electric', 'field', 'with', 'e', 'ec', 'our', 'general', 'treatment', 'encompassing', 'also', 'the', 'traditional', 'well', 'studied', 'ca... | [-0.14709433921299284, 0.18225687490629222, -0.027204638328587653, 0.05107584165058809, 0.004635064240249962, -0.07162186848967898, 0.04912044536691196, 0.3120793137367409, -0.22490651245772986, -0.32409397701013576, 0.009707480664411098, -0.2606978849347941, -0.04602273016658584, 0.23065750878119823, 0.027820849173361... |
706.4364 | Transverse $\Lambda^0$ polarization in inclusive photoproduction: quark
recombination model | Transverse polarization of $\Lambda^0$ hyperons in inclusive photoproduction
at x_F>0 is tackled within the framework of the quark recombination model,
which has been successfully applied to the polarization of different hyperons
in a variety of unpolarized hadron-hadron reactions. The results are compared
with recen... | hep-ph | transverse polarization of lambda0 hyperons in inclusive photoproduction at x_f0 is tackled within the framework of the quark recombination model which has been successfully applied to the polarization of different hyperons in a variety of unpolarized hadronhadron reactions the results are compared with recent experime... | [['transverse', 'polarization', 'of', 'lambda0', 'hyperons', 'in', 'inclusive', 'photoproduction', 'at', 'x_f0', 'is', 'tackled', 'within', 'the', 'framework', 'of', 'the', 'quark', 'recombination', 'model', 'which', 'has', 'been', 'successfully', 'applied', 'to', 'the', 'polarization', 'of', 'different', 'hyperons', '... | [-0.025687470343351986, 0.16740107950560437, -0.14428678171437545, 0.09516241293992304, -0.021644524589646608, -0.07895784141146578, -0.05332193054103603, 0.38967947483373183, -0.1772174728491033, -0.24080368387512863, -0.09822483937508271, -0.33759677902950597, 0.07084022955192874, 0.14844340334821027, 0.0973881042591... |
706.4365 | Multi-dimensional BSDE with Oblique Reflection and Optimal Switching | In this paper, we study a multi-dimensional backward stochastic differential
equation (BSDE) with oblique reflection, which is a BSDE reflected on the
boundary of a special unbounded convex domain along an oblique direction, and
which arises naturally in the study of optimal switching problem. The existence
of the ad... | math.PR | in this paper we study a multidimensional backward stochastic differential equation bsde with oblique reflection which is a bsde reflected on the boundary of a special unbounded convex domain along an oblique direction and which arises naturally in the study of optimal switching problem the existence of the adapted sol... | [['in', 'this', 'paper', 'we', 'study', 'a', 'multidimensional', 'backward', 'stochastic', 'differential', 'equation', 'bsde', 'with', 'oblique', 'reflection', 'which', 'is', 'a', 'bsde', 'reflected', 'on', 'the', 'boundary', 'of', 'a', 'special', 'unbounded', 'convex', 'domain', 'along', 'an', 'oblique', 'direction', ... | [-0.13524811579791698, 0.004852577360900112, -0.10044810971490635, 0.07599215392048593, -0.14971695347218017, -0.13343898705098517, 0.03825546901532297, 0.31884403637422665, -0.3743942007278056, -0.2336547618493611, 0.1819638825949397, -0.24053137590061843, -0.14948165918115613, 0.20567207112042016, -0.0968876738361148... |
706.4366 | Gauge-independent Abelian mechanism of color confinement in gluodynamics | Abelian mechanism of non-Abelian color confinement is observed in a
gauge-independent way by high precision lattice Monte Carlo simulations in
gluodynamics. An Abelian gauge field is extracted with no gauge-fixing. A
static quark-antiquark potential derived from Abelian Polyakov loop correlators
gives us the same str... | hep-lat hep-ph hep-th | abelian mechanism of nonabelian color confinement is observed in a gaugeindependent way by high precision lattice monte carlo simulations in gluodynamics an abelian gauge field is extracted with no gaugefixing a static quarkantiquark potential derived from abelian polyakov loop correlators gives us the same string tens... | [['abelian', 'mechanism', 'of', 'nonabelian', 'color', 'confinement', 'is', 'observed', 'in', 'a', 'gaugeindependent', 'way', 'by', 'high', 'precision', 'lattice', 'monte', 'carlo', 'simulations', 'in', 'gluodynamics', 'an', 'abelian', 'gauge', 'field', 'is', 'extracted', 'with', 'no', 'gaugefixing', 'a', 'static', 'qu... | [-0.1534015046261055, 0.2639954246438528, -0.11760277233904497, 0.13453289322052642, -0.1184302092358274, -0.13086078448931834, -0.001792306115308556, 0.3957123977597803, -0.16537659024623663, -0.25923094114803363, 0.019120762915822286, -0.22298704812572778, -0.07561913390006673, 0.09135972014873435, -0.040735021435753... |
706.4367 | Muon spin rotation measurements of the superfluid density in fresh and
aged superconducting PuCoGa$_5$ | We have measured the temperature dependence and magnitude of the superfluid
density $\rho_{\rm s}(T)$ via the magnetic field penetration depth $\lambda(T)$
in PuCoGa$_5$ (nominal critical temperature $T_{c0} = 18.5$ K) using the muon
spin rotation technique in order to investigate the symmetry of the order
parameter,... | cond-mat.str-el cond-mat.supr-con | we have measured the temperature dependence and magnitude of the superfluid density rho_rm st via the magnetic field penetration depth lambdat in pucoga_5 nominal critical temperature t_c0 185 k using the muon spin rotation technique in order to investigate the symmetry of the order parameter and to study the effects o... | [['we', 'have', 'measured', 'the', 'temperature', 'dependence', 'and', 'magnitude', 'of', 'the', 'superfluid', 'density', 'rho_rm', 'st', 'via', 'the', 'magnetic', 'field', 'penetration', 'depth', 'lambdat', 'in', 'pucoga_5', 'nominal', 'critical', 'temperature', 't_c0', '185', 'k', 'using', 'the', 'muon', 'spin', 'rot... | [-0.12054218403983884, 0.26312740151644937, -0.06149380092793507, 0.02131748051608461, -0.007887920049649335, -0.09440107697420223, 0.09596558227998478, 0.336088364559064, -0.24467412045526649, -0.3435186136438662, 0.04178336777927878, -0.35110534037167795, -0.0009793953295284047, 0.16831776346107888, 0.050990596076914... |
706.4368 | Combinatorial and geometric methods in topology | Starting from the (apparently) elementary problem of deciding how many
different topological spaces can be obtained by gluing together in pairs the
faces of an octahedron, we will describe the central role played by hyperbolic
geometry within three-dimensional topology. We will also point out the striking
difference ... | math.GT | starting from the apparently elementary problem of deciding how many different topological spaces can be obtained by gluing together in pairs the faces of an octahedron we will describe the central role played by hyperbolic geometry within threedimensional topology we will also point out the striking difference with th... | [['starting', 'from', 'the', 'apparently', 'elementary', 'problem', 'of', 'deciding', 'how', 'many', 'different', 'topological', 'spaces', 'can', 'be', 'obtained', 'by', 'gluing', 'together', 'in', 'pairs', 'the', 'faces', 'of', 'an', 'octahedron', 'we', 'will', 'describe', 'the', 'central', 'role', 'played', 'by', 'hy... | [-0.1159426351445482, 0.11476583206757296, -0.10078615238154798, 0.06930412018156953, -0.06544335529600319, -0.07481500878930092, 0.00504945277383453, 0.37187382814131287, -0.3098520397355682, -0.2987335109347968, 0.11188972015148274, -0.28824300823831245, -0.18821571887498353, 0.23158312776113713, -0.12462815063037469... |
706.4369 | The role of HST in the study of near- and mid-infrared-selected galaxies | Because of their unique quality, Hubble Space Telescope (HST) data have
played an important complementary role in studies of infrared (IR) galaxies
conducted with major facilities, as VLT or Spitzer, and will be as well very
valuable for future telescopes as Herschel and ALMA. I review here some of the
most recent wo... | astro-ph | because of their unique quality hubble space telescope hst data have played an important complementary role in studies of infrared ir galaxies conducted with major facilities as vlt or spitzer and will be as well very valuable for future telescopes as herschel and alma i review here some of the most recent works led by... | [['because', 'of', 'their', 'unique', 'quality', 'hubble', 'space', 'telescope', 'hst', 'data', 'have', 'played', 'an', 'important', 'complementary', 'role', 'in', 'studies', 'of', 'infrared', 'ir', 'galaxies', 'conducted', 'with', 'major', 'facilities', 'as', 'vlt', 'or', 'spitzer', 'and', 'will', 'be', 'as', 'well', ... | [-0.032248699642618055, 0.058773485549863835, -0.0965276547524679, 0.06737043352664582, -0.1582262946425804, -0.056831859077127386, 0.007499774784914085, 0.46147204263252206, -0.1351610329137267, -0.3243773315209962, 0.15670542786808386, -0.289804978466626, -0.08402921358564137, 0.23333859244926966, -0.0322820720113148... |
706.437 | Role of the exchange and correlation potential into calculating the
x-ray absorption spectra of half-metallic alloys: the case of Mn and Cu
K-edge XANES in Cu$_2$MnM (M = Al, Sn, In) Heusler alloys | This work reports a theoretical study of the x-ray absorption near-edge
structure spectra at both the Cu and the Mn K-edge in several Cu$_2$MnM (M= Al,
Sn and In) Heusler alloys. Our results show that {\it ab-initio} single-channel
multiple-scattering calculations are able of reproducing the experimental
spectra. Mor... | cond-mat.mtrl-sci cond-mat.other | this work reports a theoretical study of the xray absorption nearedge structure spectra at both the cu and the mn kedge in several cu_2mnm m al sn and in heusler alloys our results show that it abinitio singlechannel multiplescattering calculations are able of reproducing the experimental spectra moreover an extensive ... | [['this', 'work', 'reports', 'a', 'theoretical', 'study', 'of', 'the', 'xray', 'absorption', 'nearedge', 'structure', 'spectra', 'at', 'both', 'the', 'cu', 'and', 'the', 'mn', 'kedge', 'in', 'several', 'cu_2mnm', 'm', 'al', 'sn', 'and', 'in', 'heusler', 'alloys', 'our', 'results', 'show', 'that', 'it', 'abinitio', 'sin... | [-0.06547011170992033, 0.06388521286738823, -0.05936555681809624, 0.08159642141470884, -0.0056432414096482895, -0.05882601826848026, 0.04987615345917801, 0.45662079525596283, -0.2058918893267896, -0.29768416132936454, 0.009204218481132325, -0.38744734646752477, -0.15152169335511217, 0.17080396800698278, 0.0577093510234... |
706.4371 | The VIMOS-VLT Deep Survey. The dependence of clustering on galaxy
stellar mass at z~1 | Aims: We use the VVDS-Deep first-epoch data to measure the dependence of
galaxy clustering on galaxy stellar mass, at z~0.85.
Methods: We measure the projected correlation function wp(rp) for sub-samples
with 0.5<z<1.2 covering different mass ranges between 10^9 and 10^11 Msun. We
quantify in detail the observation... | astro-ph | aims we use the vvdsdeep firstepoch data to measure the dependence of galaxy clustering on galaxy stellar mass at z085 methods we measure the projected correlation function wprp for subsamples with 05z12 covering different mass ranges between 109 and 1011 msun we quantify in detail the observational selection biases us... | [['aims', 'we', 'use', 'the', 'vvdsdeep', 'firstepoch', 'data', 'to', 'measure', 'the', 'dependence', 'of', 'galaxy', 'clustering', 'on', 'galaxy', 'stellar', 'mass', 'at', 'z085', 'methods', 'we', 'measure', 'the', 'projected', 'correlation', 'function', 'wprp', 'for', 'subsamples', 'with', '05z12', 'covering', 'diffe... | [-0.05856634962003467, 0.08623142245770345, -0.06375021674441841, 0.12647450360654028, -0.07051126507971928, -0.0248337540990796, 0.04472508995688327, 0.389409966078007, -0.08943463066221602, -0.38602020847347546, 0.04341482486980001, -0.33200201030539456, 0.016302737101631343, 0.2183355271464811, 0.00187828059325803, ... |
706.4372 | Driving-dependent damping of Rabi oscillations in two-level
semiconductor systems | We propose a mechanism to explain the nature of the damping of Rabi
oscillations with increasing driving-pulse area in localized semiconductor
systems, and have suggested a general approach which describes a coherently
driven two-level system interacting with a dephasing reservoir. Present
calculations show that the ... | quant-ph | we propose a mechanism to explain the nature of the damping of rabi oscillations with increasing drivingpulse area in localized semiconductor systems and have suggested a general approach which describes a coherently driven twolevel system interacting with a dephasing reservoir present calculations show that the nonmar... | [['we', 'propose', 'a', 'mechanism', 'to', 'explain', 'the', 'nature', 'of', 'the', 'damping', 'of', 'rabi', 'oscillations', 'with', 'increasing', 'drivingpulse', 'area', 'in', 'localized', 'semiconductor', 'systems', 'and', 'have', 'suggested', 'a', 'general', 'approach', 'which', 'describes', 'a', 'coherently', 'driv... | [-0.17656404322716063, 0.17721160092925722, -0.06673201346873409, 0.059439805714646354, 0.008454052438200623, -0.164482934672075, 0.036778943096848066, 0.3689195987320057, -0.2287346882469676, -0.2886031490957571, 0.021674177737656498, -0.254487346323138, -0.14668640669831937, 0.24860637278632364, -0.007239400124591257... |
706.4373 | Neutrino Mixing based on Mass Matrices with a $2 \leftrightarrow 3$
Symmetry | Under the assumption that the $2\leftrightarrow 3$ symmetry is broken only
through phases, we give a systematical investigation of possible lepton mass
matrix forms without referring to the explicit parameter values. The two types
of the $2\leftrightarrow 3$ symmetry are investigated: one is that the left-
and right-... | hep-ph | under the assumption that the 2leftrightarrow 3 symmetry is broken only through phases we give a systematical investigation of possible lepton mass matrix forms without referring to the explicit parameter values the two types of the 2leftrightarrow 3 symmetry are investigated one is that the left and righthanded fields... | [['under', 'the', 'assumption', 'that', 'the', '2leftrightarrow', '3', 'symmetry', 'is', 'broken', 'only', 'through', 'phases', 'we', 'give', 'a', 'systematical', 'investigation', 'of', 'possible', 'lepton', 'mass', 'matrix', 'forms', 'without', 'referring', 'to', 'the', 'explicit', 'parameter', 'values', 'the', 'two',... | [-0.17233524050025903, 0.2648950994744436, 0.009351123926066553, 0.1495702198704167, -0.08608767557313148, -0.17472007453499228, 0.005774384839748291, 0.357096078315961, -0.18532124268294303, -0.25367238837265477, 0.09179339972743225, -0.2589252826796134, -0.05898371413734156, 0.10032367562279873, 0.05403600743558911, ... |
706.4374 | Filamentation instability in a quantum plasma | The growth rate of the filamentation instability triggered when a diluted
cold electron beam passes through a cold plasma is evaluated using the quantum
hydrodynamic equations. Compared with a cold fluid model, quantum effects
reduce both the unstable wave vector domain and the maximum growth rate.
Stabilization of l... | physics.plasm-ph astro-ph physics.space-ph | the growth rate of the filamentation instability triggered when a diluted cold electron beam passes through a cold plasma is evaluated using the quantum hydrodynamic equations compared with a cold fluid model quantum effects reduce both the unstable wave vector domain and the maximum growth rate stabilization of large ... | [['the', 'growth', 'rate', 'of', 'the', 'filamentation', 'instability', 'triggered', 'when', 'a', 'diluted', 'cold', 'electron', 'beam', 'passes', 'through', 'a', 'cold', 'plasma', 'is', 'evaluated', 'using', 'the', 'quantum', 'hydrodynamic', 'equations', 'compared', 'with', 'a', 'cold', 'fluid', 'model', 'quantum', 'e... | [-0.1714753470137373, 0.2309375361207573, -0.04637626291991308, 0.0476870918311928, -0.05773592348499545, -0.12861485040650286, -0.011224703744171593, 0.2838461183000827, -0.2615890448549013, -0.22643218403575063, 0.12603120214102426, -0.276903608878111, -0.04232932725685767, 0.22729351305691847, 0.054538448544583104, ... |
706.4375 | A Robust Linguistic Platform for Efficient and Domain specific Web
Content Analysis | Web semantic access in specific domains calls for specialized search engines
with enhanced semantic querying and indexing capacities, which pertain both to
information retrieval (IR) and to information extraction (IE). A rich
linguistic analysis is required either to identify the relevant semantic units
to index and ... | cs.AI | web semantic access in specific domains calls for specialized search engines with enhanced semantic querying and indexing capacities which pertain both to information retrieval ir and to information extraction ie a rich linguistic analysis is required either to identify the relevant semantic units to index and weight t... | [['web', 'semantic', 'access', 'in', 'specific', 'domains', 'calls', 'for', 'specialized', 'search', 'engines', 'with', 'enhanced', 'semantic', 'querying', 'and', 'indexing', 'capacities', 'which', 'pertain', 'both', 'to', 'information', 'retrieval', 'ir', 'and', 'to', 'information', 'extraction', 'ie', 'a', 'rich', 'l... | [-0.06130411632180418, 0.015104359938473639, -0.04724264639263896, 0.08452104951015516, -0.22815146668230452, -0.15907803041962523, 0.07278962490509251, 0.42895959028081126, -0.31961917014129154, -0.3563537258106246, 0.10027270103973808, -0.2990317778448153, -0.08630464856444271, 0.18386325307990972, -0.117091656397001... |
706.4376 | Transmission-line networks cloaking objects from electromagnetic fields | We consider a novel method of cloaking objects from the surrounding
electromagnetic fields in the microwave region. The method is based on
transmission-line networks that simulate the wave propagation in the medium
surrounding the cloaked object. The electromagnetic fields from the surrounding
medium are coupled into... | physics.class-ph | we consider a novel method of cloaking objects from the surrounding electromagnetic fields in the microwave region the method is based on transmissionline networks that simulate the wave propagation in the medium surrounding the cloaked object the electromagnetic fields from the surrounding medium are coupled into the ... | [['we', 'consider', 'a', 'novel', 'method', 'of', 'cloaking', 'objects', 'from', 'the', 'surrounding', 'electromagnetic', 'fields', 'in', 'the', 'microwave', 'region', 'the', 'method', 'is', 'based', 'on', 'transmissionline', 'networks', 'that', 'simulate', 'the', 'wave', 'propagation', 'in', 'the', 'medium', 'surround... | [-0.15181045919472788, 0.10980372039624921, -0.016816671719245703, -0.03908165671322265, -0.13511549552649627, -0.11161005951717128, -0.019993185088682322, 0.44411037440331264, -0.2458816399268898, -0.2872459589285247, 0.07054391756573301, -0.29111412861441943, -0.13832385449405807, 0.164678264659381, 0.005562830828115... |
706.4377 | Discovery of the Pre-Main Sequence Population of the Stellar Association
LH 95 in the Large Magellanic Cloud with Hubble Space Telescope ACS
Observations | We report the discovery of an extraordinary number of pre-main sequence (PMS)
stars in the vicinity of the stellar association LH 95 in the Large Magellanic
Cloud (LMC). Using the {\em Advanced Camera for Surveys} on-board the {\em
Hubble} Space Telescope in wide-field mode we obtained deep high-resolution
imaging of... | astro-ph | we report the discovery of an extraordinary number of premain sequence pms stars in the vicinity of the stellar association lh 95 in the large magellanic cloud lmc using the em advanced camera for surveys onboard the em hubble space telescope in widefield mode we obtained deep highresolution imaging of the main body of... | [['we', 'report', 'the', 'discovery', 'of', 'an', 'extraordinary', 'number', 'of', 'premain', 'sequence', 'pms', 'stars', 'in', 'the', 'vicinity', 'of', 'the', 'stellar', 'association', 'lh', '95', 'in', 'the', 'large', 'magellanic', 'cloud', 'lmc', 'using', 'the', 'em', 'advanced', 'camera', 'for', 'surveys', 'onboard... | [-0.07261432633394349, 0.1247840169088221, -0.07067395421413429, 0.08873364984271737, -0.14067263162859747, -0.021115801078779847, 0.17092819847043997, 0.3918608634344984, -0.1427129275242366, -0.39003611373315167, 0.01744370668643025, -0.2800555880444401, -0.009689018018900207, 0.18700391363851618, -0.0748044898830695... |
706.4378 | Magnetic solutions in AdS$_5$ and trace anomalies | We discuss black hole and black string solutions in d=5 Einstein-Yang-Mills
theory with negative cosmological constant, proposing a method to compute their
mass and action. The magnetic gauge field of these configurations does not
vanish at infinity. We argue that this implies a nonvanishing trace for the
stress tens... | hep-th | we discuss black hole and black string solutions in d5 einsteinyangmills theory with negative cosmological constant proposing a method to compute their mass and action the magnetic gauge field of these configurations does not vanish at infinity we argue that this implies a nonvanishing trace for the stress tensor of th... | [['we', 'discuss', 'black', 'hole', 'and', 'black', 'string', 'solutions', 'in', 'd5', 'einsteinyangmills', 'theory', 'with', 'negative', 'cosmological', 'constant', 'proposing', 'a', 'method', 'to', 'compute', 'their', 'mass', 'and', 'action', 'the', 'magnetic', 'gauge', 'field', 'of', 'these', 'configurations', 'does... | [-0.19096278445795178, 0.16164583716265582, -0.054443687049637514, 0.11281416988371078, -0.09742245474761282, -0.16570301577276378, -0.01754086511640775, 0.2982503850771873, -0.1639109638830026, -0.24956470081168744, 0.07940275645254317, -0.26124551656000594, -0.1458408071193844, 0.08153293704338095, -0.041947802390765... |
706.4379 | Quartic equations and 2-division on elliptic curves | Let K be a field of characteristic different from 2 and C an elliptic curve
over K given by a Weierstrass equation. To divide an element of the group C by
2, one must solve a certain quartic equation. We characterise the quartics
arising from this procedure and find how far the quartic determines the curve
and the po... | math.AG | let k be a field of characteristic different from 2 and c an elliptic curve over k given by a weierstrass equation to divide an element of the group c by 2 one must solve a certain quartic equation we characterise the quartics arising from this procedure and find how far the quartic determines the curve and the point w... | [['let', 'k', 'be', 'a', 'field', 'of', 'characteristic', 'different', 'from', '2', 'and', 'c', 'an', 'elliptic', 'curve', 'over', 'k', 'given', 'by', 'a', 'weierstrass', 'equation', 'to', 'divide', 'an', 'element', 'of', 'the', 'group', 'c', 'by', '2', 'one', 'must', 'solve', 'a', 'certain', 'quartic', 'equation', 'we... | [-0.1629678328995997, 0.057420883674085585, -0.11245896559173488, 0.027336383824904432, -0.06991792774214498, -0.15041029549045665, 0.013448706318466168, 0.29922663104140534, -0.34845255627209004, -0.26717490416441886, 0.08986793548079594, -0.29804617524990495, -0.15234070694302473, 0.24195424263708223, -0.077081077855... |
706.438 | Prospects of Jet Tomography Using Hard Processes inside a Soft Medium | The term 'tomography' is commonly applied to the idea of studying properties
of a medium by the modifications this medium induces to a known probe
propagating through it. In the context of ultrarelativistic heavy-ion
collisions, rare high transverse momentum (p_T) processes taking place
alongside soft bulk-matter pro... | hep-ph | the term tomography is commonly applied to the idea of studying properties of a medium by the modifications this medium induces to a known probe propagating through it in the context of ultrarelativistic heavyion collisions rare high transverse momentum p_t processes taking place alongside soft bulkmatter production ca... | [['the', 'term', 'tomography', 'is', 'commonly', 'applied', 'to', 'the', 'idea', 'of', 'studying', 'properties', 'of', 'a', 'medium', 'by', 'the', 'modifications', 'this', 'medium', 'induces', 'to', 'a', 'known', 'probe', 'propagating', 'through', 'it', 'in', 'the', 'context', 'of', 'ultrarelativistic', 'heavyion', 'co... | [-0.08268812977239959, 0.20455625153739343, -0.15213803965411105, 0.1371258837162758, -0.020737519715684695, -0.06890348121654112, -0.05995225593841706, 0.36069151999467947, -0.30030249892831684, -0.3167024914149221, 0.033550769108562514, -0.27986245074185667, -0.0032067730032897496, 0.14631098440222048, 0.052784866589... |
706.4381 | Neutrino Emission From Direct Urca Processes in Pion Condensed Quark
Matter | We study neutrino emission from direct Urca processes in pion condensed quark
matter. In compact stars with high baryon density, the emission is dominated by
the gapless modes of the pion condensation which leads to an enhanced
emissivity. While for massless quarks the enhancement is not remarkable, the
emissivity is... | hep-ph astro-ph nucl-th | we study neutrino emission from direct urca processes in pion condensed quark matter in compact stars with high baryon density the emission is dominated by the gapless modes of the pion condensation which leads to an enhanced emissivity while for massless quarks the enhancement is not remarkable the emissivity is signi... | [['we', 'study', 'neutrino', 'emission', 'from', 'direct', 'urca', 'processes', 'in', 'pion', 'condensed', 'quark', 'matter', 'in', 'compact', 'stars', 'with', 'high', 'baryon', 'density', 'the', 'emission', 'is', 'dominated', 'by', 'the', 'gapless', 'modes', 'of', 'the', 'pion', 'condensation', 'which', 'leads', 'to',... | [-0.039279782213270664, 0.3530139492853404, -0.07883536263715285, 0.1319203496662876, -0.0699460493424573, -0.06642287413183695, 0.05694012165529271, 0.3354294113814831, -0.1532800606189248, -0.27786048628294313, -0.05544732820738155, -0.33777621049338424, 0.02996444177383987, 0.14789064659868392, 0.057545058778487146,... |
706.4382 | Inclusive Jet Production in Photon-Photon Collisions at sqrt(s_ee) from
189 to 209 GeV | Inclusive jet production (e+e- -> e+e- +jet+X) is studied in collisions of
quasi-real photons radiated by the LEP beams at e+e- centre-of-mass energies
sqrt see from 189 to 209 GeV. Jets are reconstructed using the kp jet
algorithm. The inclusive differential cross-section is measured as a function
of the jet transve... | hep-ex | inclusive jet production ee ee jetx is studied in collisions of quasireal photons radiated by the lep beams at ee centreofmass energies sqrt see from 189 to 209 gev jets are reconstructed using the kp jet algorithm the inclusive differential crosssection is measured as a function of the jet transverse momentum ptjet in... | [['inclusive', 'jet', 'production', 'ee', 'ee', 'jetx', 'is', 'studied', 'in', 'collisions', 'of', 'quasireal', 'photons', 'radiated', 'by', 'the', 'lep', 'beams', 'at', 'ee', 'centreofmass', 'energies', 'sqrt', 'see', 'from', '189', 'to', '209', 'gev', 'jets', 'are', 'reconstructed', 'using', 'the', 'kp', 'jet', 'algo... | [-0.07541483501246309, 0.19842867045389379, -0.06858719325460055, 0.1595090984558577, 0.011587101530612392, -0.07868552475428099, -0.06368684940697515, 0.37929771945757024, -0.17800024887546897, -0.36240228048580536, -0.10986007412703817, -0.4061017065144637, 0.2107866447638063, 0.18312156799742405, 0.12194397383752992... |
706.4383 | Gauge invariant Boltzmann equation and the fluid limit | This article investigates the collisionless Boltzmann equation up to second
order in the cosmological perturbations. It describes the gauge dependence of
the distribution function and the construction of a gauge invariant
distribution function and brightness, and then derives the gauge invariant
fluid limit.
| gr-qc astro-ph | this article investigates the collisionless boltzmann equation up to second order in the cosmological perturbations it describes the gauge dependence of the distribution function and the construction of a gauge invariant distribution function and brightness and then derives the gauge invariant fluid limit | [['this', 'article', 'investigates', 'the', 'collisionless', 'boltzmann', 'equation', 'up', 'to', 'second', 'order', 'in', 'the', 'cosmological', 'perturbations', 'it', 'describes', 'the', 'gauge', 'dependence', 'of', 'the', 'distribution', 'function', 'and', 'the', 'construction', 'of', 'a', 'gauge', 'invariant', 'dis... | [-0.1543141007856574, 0.15089356331804463, -0.16514142917274216, 0.09528319590432613, -0.084893706969397, -0.039200610069687974, -0.04135293437731127, 0.2542156921699643, -0.2828142347117496, -0.315041632738051, 0.010087148337841554, -0.2565924517463806, -0.12121715310008027, 0.04529501574633773, 0.0009993756254918355,... |
706.4384 | Resistance without resistors: An anomaly | The elementary 2-terminal network consisting of a resistively ($R-$) shunted
inductance ($L$) in series with a capacitatively ($C-$) shunted resistance
($R$) with $R = \sqrt{L/C}$, is known for its non-dispersive dissipative
response, $i.e.,$ with the input impedance $Z_0(\omega) = R$, independent of
the frequency ($... | cond-mat.dis-nn cond-mat.mes-hall | the elementary 2terminal network consisting of a resistively r shunted inductance l in series with a capacitatively c shunted resistance r with r sqrtlc is known for its nondispersive dissipative response ie with the input impedance z_0omega r independent of the frequency omega in this communication we examine the prop... | [['the', 'elementary', '2terminal', 'network', 'consisting', 'of', 'a', 'resistively', 'r', 'shunted', 'inductance', 'l', 'in', 'series', 'with', 'a', 'capacitatively', 'c', 'shunted', 'resistance', 'r', 'with', 'r', 'sqrtlc', 'is', 'known', 'for', 'its', 'nondispersive', 'dissipative', 'response', 'ie', 'with', 'the',... | [-0.2085637098407363, 0.1014453722564018, -0.025321325833503317, -0.017659600021038703, -0.04474897345622633, -0.23435175028022, 0.06444600280710461, 0.3292842923519127, -0.3090245402941012, -0.22109734441059078, 0.07101361464941251, -0.25819950373743705, -0.1298149382140871, 0.1680197555622843, -0.046721694039437364, ... |
706.4385 | The chiral and flavour projection of Dirac-Kahler fermions in the
geometric discretization | It is shown that an exact chiral symmetry can be described for Dirac-Kahler
fermions using the two complexes of the geometric discretization. This
principle is extended to describe exact flavour projection and it is shown that
this necessitates the introduction of a new operator and two new structures of
complex. To ... | hep-lat | it is shown that an exact chiral symmetry can be described for dirackahler fermions using the two complexes of the geometric discretization this principle is extended to describe exact flavour projection and it is shown that this necessitates the introduction of a new operator and two new structures of complex to descr... | [['it', 'is', 'shown', 'that', 'an', 'exact', 'chiral', 'symmetry', 'can', 'be', 'described', 'for', 'dirackahler', 'fermions', 'using', 'the', 'two', 'complexes', 'of', 'the', 'geometric', 'discretization', 'this', 'principle', 'is', 'extended', 'to', 'describe', 'exact', 'flavour', 'projection', 'and', 'it', 'is', 's... | [-0.12661313797639778, 0.1758601925269035, -0.09687441107458793, 0.08921895900036758, -0.08610626049220371, -0.1348842770123902, -0.04491637099402933, 0.38737170551067746, -0.26334186958578915, -0.22555815731772247, 0.0884897416167988, -0.20734473270101425, -0.14446161932741794, 0.12199545494065835, -0.0385005614565064... |
706.4386 | The order-disorder transition in colloidal suspensions under shear flow | We study the order-disorder transition in colloidal suspensions under shear
flow by performing Brownian dynamics simulations. We characterize the
transition in terms of a statistical property of time-dependent maximum value
of the structure factor. We find that its power spectrum exhibits the power-law
behaviour only... | cond-mat.stat-mech cond-mat.soft | we study the orderdisorder transition in colloidal suspensions under shear flow by performing brownian dynamics simulations we characterize the transition in terms of a statistical property of timedependent maximum value of the structure factor we find that its power spectrum exhibits the powerlaw behaviour only in the... | [['we', 'study', 'the', 'orderdisorder', 'transition', 'in', 'colloidal', 'suspensions', 'under', 'shear', 'flow', 'by', 'performing', 'brownian', 'dynamics', 'simulations', 'we', 'characterize', 'the', 'transition', 'in', 'terms', 'of', 'a', 'statistical', 'property', 'of', 'timedependent', 'maximum', 'value', 'of', '... | [-0.18070767693519238, 0.20584164490286685, -0.11060472320222968, -0.0021313654326633375, 0.028929554835946263, -0.0871729307477893, 0.039917965201495945, 0.358886000476306, -0.25838058193131713, -0.27336561540731147, 0.058436658158249964, -0.3091473865641069, -0.13809253392104484, 0.16189906563421216, 0.03999996363315... |
706.4387 | Particle Ratios at High p_T at LHC Energies | Hadron production has been calculated in a pQCD improved parton model for pp,
dA and heavy ion collisions. We applied KKP and AKK fragmentation functions.
Our jet fragmentation study shows, that hadron ratios at high p_T depend on
quark contribution mostly and less on the gluonic one. This finding can be seen
in jet-... | hep-ph | hadron production has been calculated in a pqcd improved parton model for pp da and heavy ion collisions we applied kkp and akk fragmentation functions our jet fragmentation study shows that hadron ratios at high p_t depend on quark contribution mostly and less on the gluonic one this finding can be seen in jetenergy l... | [['hadron', 'production', 'has', 'been', 'calculated', 'in', 'a', 'pqcd', 'improved', 'parton', 'model', 'for', 'pp', 'da', 'and', 'heavy', 'ion', 'collisions', 'we', 'applied', 'kkp', 'and', 'akk', 'fragmentation', 'functions', 'our', 'jet', 'fragmentation', 'study', 'shows', 'that', 'hadron', 'ratios', 'at', 'high', ... | [-0.011219009520977529, 0.25415934910092297, -0.21064019006573492, 0.17268175910349884, 0.04109221288106508, -0.08088455186872226, -0.07616842873135789, 0.3944217755633872, -0.13508572850534822, -0.22030246085665162, -0.09010483564957718, -0.3471332111706336, 0.10457871177802897, 0.13583027036576015, 0.0801420689658698... |
706.4388 | A precessing accretion disc in the intermediate polar XY Ari? | XY Ari is the only intermediate polar to show deep X-ray eclipses of its
white dwarf. Previously published observations with Ginga and Chandra have also
revealed a broad X-ray orbital modulation, roughly antiphased with the eclipse,
and presumed to be due to absorption in an extended structure near the edge of
an acc... | astro-ph | xy ari is the only intermediate polar to show deep xray eclipses of its white dwarf previously published observations with ginga and chandra have also revealed a broad xray orbital modulation roughly antiphased with the eclipse and presumed to be due to absorption in an extended structure near the edge of an accretion ... | [['xy', 'ari', 'is', 'the', 'only', 'intermediate', 'polar', 'to', 'show', 'deep', 'xray', 'eclipses', 'of', 'its', 'white', 'dwarf', 'previously', 'published', 'observations', 'with', 'ginga', 'and', 'chandra', 'have', 'also', 'revealed', 'a', 'broad', 'xray', 'orbital', 'modulation', 'roughly', 'antiphased', 'with', ... | [-0.12513414035272885, 0.10183548164179994, -0.08802974725836317, 0.07261680443066677, -0.10481678424712366, -0.111052858550123, 0.033003672003115415, 0.4761012243072595, -0.24196627947099755, -0.34016822424555726, 0.11506827535087112, -0.30660480399247914, -0.07433268136123189, 0.20547525101681532, -0.0663452924682837... |
706.4389 | Calculation of the atmospheric muon flux motivated by the ATIC-2
experiment | We calculate the cosmic ray muon flux at ground level using directly the
primary cosmic ray spectrum and composition measured in the ATIC-2 balloon
experiment. In order to extend the calculations to high energies, up to 100
TeV, we use the data of the GAMMA experiment as well as Zatsepin and Sokolskaya
model. This mo... | astro-ph hep-ex | we calculate the cosmic ray muon flux at ground level using directly the primary cosmic ray spectrum and composition measured in the atic2 balloon experiment in order to extend the calculations to high energies up to 100 tev we use the data of the gamma experiment as well as zatsepin and sokolskaya model this model sup... | [['we', 'calculate', 'the', 'cosmic', 'ray', 'muon', 'flux', 'at', 'ground', 'level', 'using', 'directly', 'the', 'primary', 'cosmic', 'ray', 'spectrum', 'and', 'composition', 'measured', 'in', 'the', 'atic2', 'balloon', 'experiment', 'in', 'order', 'to', 'extend', 'the', 'calculations', 'to', 'high', 'energies', 'up',... | [-0.02909351024985105, 0.18409186975470374, -0.020890706217557946, 0.1562068364908593, -0.033626080106396776, -0.03581981955525967, 0.0009277847797407971, 0.3388620503637549, -0.21962155532938513, -0.3953173915249901, 0.027990278163501484, -0.3803362762099588, 0.0226768234718617, 0.25053527471088394, 0.0630161985724438... |
706.439 | On Hamiltonian stationary Lagrangian spheres in non-Einstein Kaehler
surfaces | Hamiltonian stationary Lagrangian spheres in Kaehler-Einstein surfaces are
minimal. We prove that in the family of non-Einstein Kaehler surfaces given by
the product $\Sigma_1\times\Sigma_2$ of two complete orientable Riemannian
surfaces of different constant Gauss curvatures, there is only a (non minimal)
Hamiltonia... | math.DG | hamiltonian stationary lagrangian spheres in kaehlereinstein surfaces are minimal we prove that in the family of noneinstein kaehler surfaces given by the product sigma_1timessigma_2 of two complete orientable riemannian surfaces of different constant gauss curvatures there is only a non minimal hamiltonian stationary ... | [['hamiltonian', 'stationary', 'lagrangian', 'spheres', 'in', 'kaehlereinstein', 'surfaces', 'are', 'minimal', 'we', 'prove', 'that', 'in', 'the', 'family', 'of', 'noneinstein', 'kaehler', 'surfaces', 'given', 'by', 'the', 'product', 'sigma_1timessigma_2', 'of', 'two', 'complete', 'orientable', 'riemannian', 'surfaces'... | [-0.27341789038230974, 0.16294760593180463, -0.02142994288812604, 0.1063011266850752, -0.07078231054178455, -0.20587610629011402, -0.0943298452072205, 0.37955092150195124, -0.2085702173705948, -0.2340872193964427, 0.06718060395909115, -0.3130195128420989, -0.16654184102816016, 0.1536803128638942, -0.13848914853052088, ... |
706.4391 | Cavity method for quantum spin glasses on the Bethe lattice | We propose a generalization of the cavity method to quantum spin glasses on
fixed connectivity lattices. Our work is motivated by the recent refinements of
the classical technique and its potential application to quantum computational
problems. We numerically solve for the phase structure of a connectivity $q=3$
tran... | cond-mat.stat-mech cond-mat.dis-nn | we propose a generalization of the cavity method to quantum spin glasses on fixed connectivity lattices our work is motivated by the recent refinements of the classical technique and its potential application to quantum computational problems we numerically solve for the phase structure of a connectivity q3 transverse ... | [['we', 'propose', 'a', 'generalization', 'of', 'the', 'cavity', 'method', 'to', 'quantum', 'spin', 'glasses', 'on', 'fixed', 'connectivity', 'lattices', 'our', 'work', 'is', 'motivated', 'by', 'the', 'recent', 'refinements', 'of', 'the', 'classical', 'technique', 'and', 'its', 'potential', 'application', 'to', 'quantu... | [-0.13881101299995097, 0.13611921352212844, -0.07523867641778095, 0.02946275242678551, -0.054360071200526494, -0.14166942820546852, 0.06272828623996643, 0.37013755457988684, -0.26351852017873223, -0.27520959800028283, 0.07552217544002486, -0.25488971362727275, -0.17075966287782227, 0.17755231530864493, -0.0054004058322... |
706.4392 | Vector Meson production from NLL BFKL | The amplitude for the forward electroproduction of two light vector mesons
can be written completely within perturbative QCD in the Regge limit with
next-to-leading accuracy, thus providing the first example of a physical
application of the BFKL approach at the next-to-leading order. We study in the
case of equal pho... | hep-ph | the amplitude for the forward electroproduction of two light vector mesons can be written completely within perturbative qcd in the regge limit with nexttoleading accuracy thus providing the first example of a physical application of the bfkl approach at the nexttoleading order we study in the case of equal photon virt... | [['the', 'amplitude', 'for', 'the', 'forward', 'electroproduction', 'of', 'two', 'light', 'vector', 'mesons', 'can', 'be', 'written', 'completely', 'within', 'perturbative', 'qcd', 'in', 'the', 'regge', 'limit', 'with', 'nexttoleading', 'accuracy', 'thus', 'providing', 'the', 'first', 'example', 'of', 'a', 'physical', ... | [-0.10516028301003323, 0.12881392559272722, -0.15762959898803647, 0.09520357729158771, -0.03460030950291056, -0.04492249162736493, 0.04853229376841599, 0.32794292276384124, -0.1943399076756667, -0.24355694683085025, 0.012261457114913304, -0.29119072211775143, -0.04448032688716767, 0.1442042755776308, 0.0570594950572548... |
706.4393 | $\bar{K}NN$ quasi-bound state and the $\bar{K}N$ interaction:
coupled-channel Faddeev calculations of the $\bar{K}NN - \pi \Sigma N$ system | Coupled-channel three-body calculations of an $I=1/2$, $J^{\pi}=0^-$
$\bar{K}NN$ quasi-bound state in the $\bar{K}NN - \pi \Sigma N$ system were
performed and the dependence of the resulting three-body energy on the two-body
$\bar{K}N - \pi \Sigma$ interaction was investigated. Earlier results of
binding energy $B_{K... | nucl-th | coupledchannel threebody calculations of an i12 jpi0 barknn quasibound state in the barknn pi sigma n system were performed and the dependence of the resulting threebody energy on the twobody barkn pi sigma interaction was investigated earlier results of binding energy b_kpp sim 50 70 mev and width gamma_kpp sim 100 me... | [['coupledchannel', 'threebody', 'calculations', 'of', 'an', 'i12', 'jpi0', 'barknn', 'quasibound', 'state', 'in', 'the', 'barknn', 'pi', 'sigma', 'n', 'system', 'were', 'performed', 'and', 'the', 'dependence', 'of', 'the', 'resulting', 'threebody', 'energy', 'on', 'the', 'twobody', 'barkn', 'pi', 'sigma', 'interaction... | [-0.10259102373953631, 0.1884746653874011, -0.030111216662570515, 0.0359872234712771, -0.013085771875302406, -0.16626314321493216, 0.08793760704847568, 0.3304809906242534, -0.0971861068218788, -0.32128785613012756, -0.16162430908545813, -0.3746278764719659, -0.05436585968771474, 0.12761382536189828, 0.11225219187079037... |
706.4394 | Improvements on removing non-optimal support points in D-optimum design
algorithms | We improve the inequality used in Pronzato [2003. Removing non-optimal
support points in D-optimum design algorithms. Statist. Probab. Lett. 63,
223-228] to remove points from the design space during the search for a
$D$-optimum design. Let $\xi$ be any design on a compact space $\mathcal{X}
\subset \mathbb{R}^m$ wit... | math.ST stat.TH | we improve the inequality used in pronzato 2003 removing nonoptimal support points in doptimum design algorithms statist probab lett 63 223228 to remove points from the design space during the search for a doptimum design let xi be any design on a compact space mathcalx subset mathbbrm with a nonsingular information ma... | [['we', 'improve', 'the', 'inequality', 'used', 'in', 'pronzato', '2003', 'removing', 'nonoptimal', 'support', 'points', 'in', 'doptimum', 'design', 'algorithms', 'statist', 'probab', 'lett', '63', '223228', 'to', 'remove', 'points', 'from', 'the', 'design', 'space', 'during', 'the', 'search', 'for', 'a', 'doptimum', '... | [-0.08976511911044384, 0.04978028577458751, -0.08818209318125302, 0.015172131858799641, -0.0997952895536851, -0.15319328143907426, 0.08107041830494832, 0.34965441986784207, -0.2565561686013196, -0.24261515498631173, 0.10455979195398253, -0.25268175635856016, -0.1713204973855534, 0.21456416231278028, -0.1595305708732019... |
706.4395 | The distribution of free path lengths in the periodic Lorentz gas and
related lattice point problems | The periodic Lorentz gas describes the dynamics of a point particle in a
periodic array of spherical scatterers, and is one of the fundamental models
for chaotic diffusion. In the present paper we investigate the Boltzmann-Grad
limit, where the radius of each scatterer tends to zero, and prove the
existence of a limi... | math.DS math-ph math.MP math.NT | the periodic lorentz gas describes the dynamics of a point particle in a periodic array of spherical scatterers and is one of the fundamental models for chaotic diffusion in the present paper we investigate the boltzmanngrad limit where the radius of each scatterer tends to zero and prove the existence of a limiting di... | [['the', 'periodic', 'lorentz', 'gas', 'describes', 'the', 'dynamics', 'of', 'a', 'point', 'particle', 'in', 'a', 'periodic', 'array', 'of', 'spherical', 'scatterers', 'and', 'is', 'one', 'of', 'the', 'fundamental', 'models', 'for', 'chaotic', 'diffusion', 'in', 'the', 'present', 'paper', 'we', 'investigate', 'the', 'b... | [-0.16149510635566616, 0.16073776988940702, -0.08434842471141628, 0.050125951839470155, -0.0020857614892816475, -0.09556115595190677, 0.03468148976288259, 0.341646222592613, -0.29305897171197587, -0.19613627704986653, 0.11342561835163208, -0.2777270546161331, -0.122086692720565, 0.15965608059737268, -0.0316753059978932... |
706.4396 | Silver staining of proteins in polyacrylamide gels | Silver staining is used to detect proteins after electrophoretic separation
on polyacrylamide gels. It combines excellent sensitivity (in the low nanogram
range) with the use of very simple and cheap equipment and chemicals. It is
compatible with downstream processing, such as mass spectrometry analysis after
protein... | q-bio.GN | silver staining is used to detect proteins after electrophoretic separation on polyacrylamide gels it combines excellent sensitivity in the low nanogram range with the use of very simple and cheap equipment and chemicals it is compatible with downstream processing such as mass spectrometry analysis after protein digest... | [['silver', 'staining', 'is', 'used', 'to', 'detect', 'proteins', 'after', 'electrophoretic', 'separation', 'on', 'polyacrylamide', 'gels', 'it', 'combines', 'excellent', 'sensitivity', 'in', 'the', 'low', 'nanogram', 'range', 'with', 'the', 'use', 'of', 'very', 'simple', 'and', 'cheap', 'equipment', 'and', 'chemicals'... | [-0.005783942191538319, 0.17284506568413915, -0.05731158672822911, 0.015345710224598574, 0.016983454737324013, -0.1952358617863247, 0.0347656965870591, 0.47099414804172746, -0.263607806652712, -0.30530373040514375, 0.12278812726873688, -0.2663826242776461, -0.15469058733676488, 0.18867240778342323, -0.06315826312005882... |
706.4397 | Egorov property in perturbed cat map | We study the time evolution of the quantum-classical correspondence (QCC) for
the well known model of quantised perturbed cat maps on the torus in the very
specific regime of semi-classically small perturbations. The quality of the QCC
is measured by the overlap of classical phase-space density and corresponding
Wign... | quant-ph | we study the time evolution of the quantumclassical correspondence qcc for the well known model of quantised perturbed cat maps on the torus in the very specific regime of semiclassically small perturbations the quality of the qcc is measured by the overlap of classical phasespace density and corresponding wigner funct... | [['we', 'study', 'the', 'time', 'evolution', 'of', 'the', 'quantumclassical', 'correspondence', 'qcc', 'for', 'the', 'well', 'known', 'model', 'of', 'quantised', 'perturbed', 'cat', 'maps', 'on', 'the', 'torus', 'in', 'the', 'very', 'specific', 'regime', 'of', 'semiclassically', 'small', 'perturbations', 'the', 'qualit... | [-0.11237534461062901, 0.13714397763329336, -0.11963666445508446, 0.13686123296027983, 0.012232475761641009, -0.13568371214625455, 0.03220974099846346, 0.27949609778360607, -0.29527906705769374, -0.24886323193078572, 0.062416843745915086, -0.23866766537107603, -0.1650613713169413, 0.17602627130810977, -0.04149966914994... |
706.4398 | Strong-Coupling Superconductivity of CeIrSi$_3$ with the
Non-centrosymmetric Crystal Structure | We studied the pressure-induced superconductor CeIrSi$_3$ with the
non-centrosymmetric tetragonal structure under high pressure. The electrical
resistivity and ac heat capacity were measured in the same run for the same
sample. The critical pressure was determined to be $P_{\rm c}$ = 2.25 GPa,
where the antiferromagn... | cond-mat.str-el | we studied the pressureinduced superconductor ceirsi_3 with the noncentrosymmetric tetragonal structure under high pressure the electrical resistivity and ac heat capacity were measured in the same run for the same sample the critical pressure was determined to be p_rm c 225 gpa where the antiferromagnetic state disapp... | [['we', 'studied', 'the', 'pressureinduced', 'superconductor', 'ceirsi_3', 'with', 'the', 'noncentrosymmetric', 'tetragonal', 'structure', 'under', 'high', 'pressure', 'the', 'electrical', 'resistivity', 'and', 'ac', 'heat', 'capacity', 'were', 'measured', 'in', 'the', 'same', 'run', 'for', 'the', 'same', 'sample', 'th... | [-0.18599318530650635, 0.22733375254028942, 0.02806153764577175, -0.038144851776451105, -0.04539297848386923, -0.1778421531082131, 0.19016858235117978, 0.35601453031413255, -0.2494332958071027, -0.3194075369858183, 0.03770282938639866, -0.3942953976802528, 0.029140274034580214, 0.16286538572312564, 0.07977322946953791,... |
706.4399 | A criterion for entanglement in two two-level systems | We prove a necessary and sufficient condition for the occurrence of
entanglement in two two-level systems, simple enough to be of experimental
interest. Our results are illustrated in the context of a spin star system
analyzing the exact entanglement evolution of the central couple of spins.
| quant-ph | we prove a necessary and sufficient condition for the occurrence of entanglement in two twolevel systems simple enough to be of experimental interest our results are illustrated in the context of a spin star system analyzing the exact entanglement evolution of the central couple of spins | [['we', 'prove', 'a', 'necessary', 'and', 'sufficient', 'condition', 'for', 'the', 'occurrence', 'of', 'entanglement', 'in', 'two', 'twolevel', 'systems', 'simple', 'enough', 'to', 'be', 'of', 'experimental', 'interest', 'our', 'results', 'are', 'illustrated', 'in', 'the', 'context', 'of', 'a', 'spin', 'star', 'system'... | [-0.17125137614936609, 0.13618310284800828, -0.057824174063685146, 0.0927192265694232, 0.006961020033644593, -0.13819887345332815, 0.004070487212511184, 0.34151616190438683, -0.1926502184132519, -0.25672292713399814, 0.1217891814885661, -0.243150574033675, -0.1083180889406282, 0.23190623151300394, -0.02764606390796278,... |
706.44 | Albert Einstein - a Pious Atheist | We consider Einstein's attitude with regard to religion both from
sociological and epistemological points of view. An attempt to put it into a
wider socio-historical perspective has been made, with the emphasis on his
ethnic and religious background. The great scientist was neither anatheist nor
a believer in the ort... | physics.hist-ph physics.gen-ph | we consider einsteins attitude with regard to religion both from sociological and epistemological points of view an attempt to put it into a wider sociohistorical perspective has been made with the emphasis on his ethnic and religious background the great scientist was neither anatheist nor a believer in the orthodox s... | [['we', 'consider', 'einsteins', 'attitude', 'with', 'regard', 'to', 'religion', 'both', 'from', 'sociological', 'and', 'epistemological', 'points', 'of', 'view', 'an', 'attempt', 'to', 'put', 'it', 'into', 'a', 'wider', 'sociohistorical', 'perspective', 'has', 'been', 'made', 'with', 'the', 'emphasis', 'on', 'his', 'e... | [-0.04272950403018123, 0.056967800426069255, -0.16306232877208718, 0.1179202092675301, -0.21956405933555548, -0.15242059884725936, 0.08825145484297536, 0.3341503869451117, -0.2200407694659329, -0.30899956022039987, 0.10479367316397006, -0.2943524344913645, -0.1629150428052526, 0.14456396104651503, -0.19441354291796284,... |
706.4401 | Dynamics of DNA-breathing: Weak noise analysis, finite time singularity,
and mapping onto the quantum Coulomb problem | We study the dynamics of denaturation bubbles in double-stranded DNA on the
basis of the Poland-Scheraga model. We show that long time distributions for
the survival of DNA bubbles and the size autocorrelation function can be
derived from an asymptotic weak noise approach. In particular, below the
melting temperature... | cond-mat.stat-mech cond-mat.soft | we study the dynamics of denaturation bubbles in doublestranded dna on the basis of the polandscheraga model we show that long time distributions for the survival of dna bubbles and the size autocorrelation function can be derived from an asymptotic weak noise approach in particular below the melting temperature the bu... | [['we', 'study', 'the', 'dynamics', 'of', 'denaturation', 'bubbles', 'in', 'doublestranded', 'dna', 'on', 'the', 'basis', 'of', 'the', 'polandscheraga', 'model', 'we', 'show', 'that', 'long', 'time', 'distributions', 'for', 'the', 'survival', 'of', 'dna', 'bubbles', 'and', 'the', 'size', 'autocorrelation', 'function', ... | [-0.12567437231593148, 0.1940502740197215, -0.12622186259865026, 0.10134696284174578, 0.017214155054165865, -0.11103331126128389, 0.04006950818756464, 0.3496342578404386, -0.3135696476928785, -0.20782285709340703, 0.04708125262396594, -0.29719656488766344, -0.08569483013010361, 0.1281214092356402, 0.02915815978506121, ... |
706.4402 | Thermal gradient-induced forces on geodetic reference masses for LISA | The low frequency sensitivity of space-borne gravitational wave observatories
will depend critically on the geodetic purity of the trajectories of orbiting
test masses. Fluctuations in the temperature difference across the enclosure
surrounding the free-falling test mass can produce noisy forces through several
proce... | gr-qc | the low frequency sensitivity of spaceborne gravitational wave observatories will depend critically on the geodetic purity of the trajectories of orbiting test masses fluctuations in the temperature difference across the enclosure surrounding the freefalling test mass can produce noisy forces through several processes ... | [['the', 'low', 'frequency', 'sensitivity', 'of', 'spaceborne', 'gravitational', 'wave', 'observatories', 'will', 'depend', 'critically', 'on', 'the', 'geodetic', 'purity', 'of', 'the', 'trajectories', 'of', 'orbiting', 'test', 'masses', 'fluctuations', 'in', 'the', 'temperature', 'difference', 'across', 'the', 'enclos... | [-0.15718050337720774, 0.1782641821861347, -0.08365947035922398, 0.0376140799527357, -0.08021241373830645, -0.04461703381140626, 0.029105070733054673, 0.32280214148904046, -0.17647759721446057, -0.3469649779019497, 0.0769142791727728, -0.2891807294006632, -0.07366786784021764, 0.26575554064500034, -0.035136640928084814... |
706.4403 | Recursion between Mumford volumes of moduli spaces | We propose a new proof, as well as a generalization of Mirzakhani's recursion
for volumes of moduli spaces. We interpret those recursion relations in terms
of expectation values in Kontsevich's integral, i.e. we relate them to a Ribbon
graph decomposition of Riemann surfaces. We find a generalization of
Mirzakhani's ... | math.AG hep-th math-ph math.MP | we propose a new proof as well as a generalization of mirzakhanis recursion for volumes of moduli spaces we interpret those recursion relations in terms of expectation values in kontsevichs integral ie we relate them to a ribbon graph decomposition of riemann surfaces we find a generalization of mirzakhanis recursions ... | [['we', 'propose', 'a', 'new', 'proof', 'as', 'well', 'as', 'a', 'generalization', 'of', 'mirzakhanis', 'recursion', 'for', 'volumes', 'of', 'moduli', 'spaces', 'we', 'interpret', 'those', 'recursion', 'relations', 'in', 'terms', 'of', 'expectation', 'values', 'in', 'kontsevichs', 'integral', 'ie', 'we', 'relate', 'the... | [-0.15852419286966324, 0.07832186382764311, -0.10437037086169888, 0.17096948119074995, -0.1388678942396959, -0.09838682684852783, 0.03833081145117532, 0.3223647719610538, -0.28825365998191455, -0.2731654479988475, 0.08942257677058954, -0.24767100644200596, -0.19940908703563817, 0.23227791527091568, -0.15898305135813834... |
706.4404 | Muon multiplicity at high energy proton-nuclei collisions | Estimation of multiplicity of muons and pions production at high energy
proton-nuclei collisions is given. Both QED and QCD contributions are
considered for peripheral kinematics of muon pair and $\sigma$-meson
production, keeping in mind it's final conversion to muons. An attempt to
explain the excess of positive ch... | hep-ph | estimation of multiplicity of muons and pions production at high energy protonnuclei collisions is given both qed and qcd contributions are considered for peripheral kinematics of muon pair and sigmameson production keeping in mind its final conversion to muons an attempt to explain the excess of positive charged muons... | [['estimation', 'of', 'multiplicity', 'of', 'muons', 'and', 'pions', 'production', 'at', 'high', 'energy', 'protonnuclei', 'collisions', 'is', 'given', 'both', 'qed', 'and', 'qcd', 'contributions', 'are', 'considered', 'for', 'peripheral', 'kinematics', 'of', 'muon', 'pair', 'and', 'sigmameson', 'production', 'keeping'... | [-0.06836437017007388, 0.25715753071697117, -0.0320515648498641, 0.1647888283738499, 0.019676132078625654, -0.09138418487763326, -0.04875927760363802, 0.32258711417058583, -0.17838359587078326, -0.3567566963580535, -0.07772422378184274, -0.42987938318401575, 0.09593080301879366, 0.1073055002427856, 0.04174888314140078,... |
706.4405 | Tightness of voter model interfaces | Consider a long-range, one-dimensional voter model started with all zeroes on
the negative integers and all ones on the positive integers. If the process
obtained by identifying states that are translations of each other is
positively recurrent, then it is said that the voter model exhibits interface
tightness. In 19... | math.PR | consider a longrange onedimensional voter model started with all zeroes on the negative integers and all ones on the positive integers if the process obtained by identifying states that are translations of each other is positively recurrent then it is said that the voter model exhibits interface tightness in 1995 cox a... | [['consider', 'a', 'longrange', 'onedimensional', 'voter', 'model', 'started', 'with', 'all', 'zeroes', 'on', 'the', 'negative', 'integers', 'and', 'all', 'ones', 'on', 'the', 'positive', 'integers', 'if', 'the', 'process', 'obtained', 'by', 'identifying', 'states', 'that', 'are', 'translations', 'of', 'each', 'other',... | [-0.12195575022146352, 0.12734326260349105, -0.07593559743143803, 0.06851820239219608, -0.05280300919428345, -0.24441924619619265, 0.06729209570460452, 0.36965248076445306, -0.2538355049746465, -0.20538096370036937, 0.10323766355060257, -0.26810729903099706, -0.15634644253194824, 0.11851364752847302, -0.037370473900732... |
706.4406 | Self-motile colloidal particles: from directed propulsion to random walk | The motion of an artificial micro-scale swimmer that uses a chemical reaction
catalyzed on its own surface to achieve autonomous propulsion is fully
characterized experimentally. It is shown that at short times, it has a
substantial component of directed motion, with a velocity that depends on the
concentration of fu... | cond-mat.soft cond-mat.stat-mech | the motion of an artificial microscale swimmer that uses a chemical reaction catalyzed on its own surface to achieve autonomous propulsion is fully characterized experimentally it is shown that at short times it has a substantial component of directed motion with a velocity that depends on the concentration of fuel mol... | [['the', 'motion', 'of', 'an', 'artificial', 'microscale', 'swimmer', 'that', 'uses', 'a', 'chemical', 'reaction', 'catalyzed', 'on', 'its', 'own', 'surface', 'to', 'achieve', 'autonomous', 'propulsion', 'is', 'fully', 'characterized', 'experimentally', 'it', 'is', 'shown', 'that', 'at', 'short', 'times', 'it', 'has', ... | [-0.1296575951533956, 0.19162702054803193, -0.10650046951923287, -0.05963581776565039, -0.053316582754058275, -0.15445919828734508, 0.01938764566837467, 0.4155467929514615, -0.269608678026615, -0.25878033492910235, 0.058833302347920835, -0.23248542225797122, -0.1723395464574232, 0.2157812113751118, -0.0583547566845817,... |
706.4407 | Supersymmetric heterotic string backgrounds | We present the main features of the solution of the gravitino and dilatino
Killing spinor equations derived in hep-th/0510176 and hep-th/0703143 which
have led to the classification of geometric types of all type I backgrounds. We
then apply these results to the supersymmetric backgrounds of the heterotic
string. In ... | hep-th | we present the main features of the solution of the gravitino and dilatino killing spinor equations derived in hepth0510176 and hepth0703143 which have led to the classification of geometric types of all type i backgrounds we then apply these results to the supersymmetric backgrounds of the heterotic string in particul... | [['we', 'present', 'the', 'main', 'features', 'of', 'the', 'solution', 'of', 'the', 'gravitino', 'and', 'dilatino', 'killing', 'spinor', 'equations', 'derived', 'in', 'hepth0510176', 'and', 'hepth0703143', 'which', 'have', 'led', 'to', 'the', 'classification', 'of', 'geometric', 'types', 'of', 'all', 'type', 'i', 'back... | [-0.10095349980983884, 0.10615397357614711, -0.05408771197544411, 0.0795423006056808, -0.14222755763621536, -0.1353165421052836, -0.05782812692341395, 0.3106343674939126, -0.18165741030243227, -0.2474515629641246, 0.07371883980413259, -0.2757545594591647, -0.17542840903624893, 0.11973358330433256, -0.06073245451552793,... |
706.4408 | Genetic embedded matching approach to ground states in continuous-spin
systems | Due to an extremely rugged structure of the free energy landscape, the
determination of spin-glass ground states is among the hardest known
optimization problems, found to be NP-hard in the most general case. Owing to
the specific structure of local (free) energy minima, general-purpose
optimization strategies perfor... | cond-mat.dis-nn cond-mat.stat-mech | due to an extremely rugged structure of the free energy landscape the determination of spinglass ground states is among the hardest known optimization problems found to be nphard in the most general case owing to the specific structure of local free energy minima generalpurpose optimization strategies perform relativel... | [['due', 'to', 'an', 'extremely', 'rugged', 'structure', 'of', 'the', 'free', 'energy', 'landscape', 'the', 'determination', 'of', 'spinglass', 'ground', 'states', 'is', 'among', 'the', 'hardest', 'known', 'optimization', 'problems', 'found', 'to', 'be', 'nphard', 'in', 'the', 'most', 'general', 'case', 'owing', 'to', ... | [-0.07278786459638094, 0.09797424162838177, -0.059858216623337394, 0.13416295098945472, -0.044807611772900116, -0.17410046656561248, 0.020724008318639416, 0.4131291879834059, -0.25622444721503757, -0.3308262190343264, 0.11751329328313552, -0.2214294458664132, -0.13285266922834768, 0.21081461324459216, -0.02822335589992... |
706.4409 | THERMINATOR simulations and PHENIX images of a heavy tail of particle
emission in 200 GeV Au+Au collisions | Correlation between emitted particles from a thermalized medium carry
important information about the space-time extent and the dynamics of the
particle emitting source. Pion emission source functions S(r) have been
measured in PHENIX using an imaging technique, and it has been found that it
contains a heavy (power-l... | nucl-th | correlation between emitted particles from a thermalized medium carry important information about the spacetime extent and the dynamics of the particle emitting source pion emission source functions sr have been measured in phenix using an imaging technique and it has been found that it contains a heavy powerlaw tail i... | [['correlation', 'between', 'emitted', 'particles', 'from', 'a', 'thermalized', 'medium', 'carry', 'important', 'information', 'about', 'the', 'spacetime', 'extent', 'and', 'the', 'dynamics', 'of', 'the', 'particle', 'emitting', 'source', 'pion', 'emission', 'source', 'functions', 'sr', 'have', 'been', 'measured', 'in'... | [-0.06026572135636921, 0.1631890498628226, -0.19416098314704316, 0.14701104676827195, -0.047556273150963314, -0.12438067672209757, -0.034656434326263315, 0.399959746093461, -0.20113400127738715, -0.2770467041455435, 0.013233856886455958, -0.3583027893733798, -0.02538734292329261, 0.1482483071670162, 0.0754962196601837,... |
706.441 | Environment-Mediated Quantum State Transfer | We propose a scheme for quantum state transfer(QST) between two qubits which
is based on their individual interaction with a common boson environment. The
corresponding single mode spin-boson Hamiltonian is solved by mapping it onto a
wave propagation problem in a semi-infinite ladder and the fidelity is
obtained. Hi... | quant-ph | we propose a scheme for quantum state transferqst between two qubits which is based on their individual interaction with a common boson environment the corresponding single mode spinboson hamiltonian is solved by mapping it onto a wave propagation problem in a semiinfinite ladder and the fidelity is obtained high fidel... | [['we', 'propose', 'a', 'scheme', 'for', 'quantum', 'state', 'transferqst', 'between', 'two', 'qubits', 'which', 'is', 'based', 'on', 'their', 'individual', 'interaction', 'with', 'a', 'common', 'boson', 'environment', 'the', 'corresponding', 'single', 'mode', 'spinboson', 'hamiltonian', 'is', 'solved', 'by', 'mapping'... | [-0.1783631576202166, 0.2381887799705577, 0.0171986008407893, 0.06291752014694345, -0.012461974107326917, -0.2380866230936882, 0.04477618044575699, 0.4058945996364878, -0.24239034840354212, -0.24335751406572484, 0.05988876749100278, -0.27658114461573186, -0.07032589935036491, 0.19949595568080744, 0.045058531456707435, ... |
706.4411 | Relaxation Enhancement by Time-Periodic Flows | We study enhancement of diffusive mixing by fast incompressible time-periodic
flows. The class of relaxation-enhancing flows that are especially efficient in
speeding up mixing has been introduced in [2]. The relaxation-enhancing
property of a flow has been shown to be intimately related to the properties of
the dyna... | math.AP math.FA math.SP | we study enhancement of diffusive mixing by fast incompressible timeperiodic flows the class of relaxationenhancing flows that are especially efficient in speeding up mixing has been introduced in 2 the relaxationenhancing property of a flow has been shown to be intimately related to the properties of the dynamical sys... | [['we', 'study', 'enhancement', 'of', 'diffusive', 'mixing', 'by', 'fast', 'incompressible', 'timeperiodic', 'flows', 'the', 'class', 'of', 'relaxationenhancing', 'flows', 'that', 'are', 'especially', 'efficient', 'in', 'speeding', 'up', 'mixing', 'has', 'been', 'introduced', 'in', '2', 'the', 'relaxationenhancing', 'p... | [-0.15803537663271724, 0.15779293031614386, -0.08679638599612932, 0.03715315094918826, -0.06824151866790977, -0.13575291519933755, -0.03780073642559435, 0.3611663781192111, -0.3035921247076543, -0.1873327585836423, 0.12318599053348105, -0.27909985454431896, -0.1612798763484555, 0.2122171006644487, -0.03412304250469924,... |
706.4412 | Optimal phase estimation in quantum networks | We address the problem of estimating the phase phi given N copies of the
phase rotation u(phi) within an array of quantum operations in finite
dimensions. We first consider the special case where the array consists of an
arbitrary input state followed by any arrangement of the N phase rotations, and
ending with a POV... | quant-ph | we address the problem of estimating the phase phi given n copies of the phase rotation uphi within an array of quantum operations in finite dimensions we first consider the special case where the array consists of an arbitrary input state followed by any arrangement of the n phase rotations and ending with a povm we o... | [['we', 'address', 'the', 'problem', 'of', 'estimating', 'the', 'phase', 'phi', 'given', 'n', 'copies', 'of', 'the', 'phase', 'rotation', 'uphi', 'within', 'an', 'array', 'of', 'quantum', 'operations', 'in', 'finite', 'dimensions', 'we', 'first', 'consider', 'the', 'special', 'case', 'where', 'the', 'array', 'consists'... | [-0.14733075498981346, 0.1563664662211126, -0.00589993170066045, -0.006135164313986529, -0.01114385187081845, -0.1460339354424931, 0.06223777948537528, 0.38076737858723886, -0.26241782162393823, -0.24557139120977556, 0.12213475477655815, -0.2591801044452788, -0.13519078007170765, 0.15834302602262043, -0.079002085651298... |
706.4413 | Quantum wave equations in curved space-time from wave mechanics | Alternative versions of the Klein-Gordon and Dirac equations in a curved
spacetime are got by applying directly the classical-quantum correspondence.
| gr-qc | alternative versions of the kleingordon and dirac equations in a curved spacetime are got by applying directly the classicalquantum correspondence | [['alternative', 'versions', 'of', 'the', 'kleingordon', 'and', 'dirac', 'equations', 'in', 'a', 'curved', 'spacetime', 'are', 'got', 'by', 'applying', 'directly', 'the', 'classicalquantum', 'correspondence']] | [-0.11826211658772082, 0.1449581203982234, -0.15336260125041007, 0.13200724464841188, -0.14799958593212068, -0.22067279235925524, -0.05249510034918785, 0.27838320694863794, -0.20431422097608448, -0.2769689353182912, 0.025072595238452778, -0.25682456865906717, -0.19514914602041245, 0.15293804230168462, -0.09356090365909... |
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