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 |
|---|---|---|---|---|---|---|
709.4135 | Effect of matrix parameters on mesoporous matrix based quantum
computation | We present a solid state implementation of quantum computation, which
improves previously proposed optically driven schemes. Our proposal is based on
vertical arrays of quantum dots embedded in a mesoporous material which can be
fabricated with present technology. We study the feasibility of performing
quantum comput... | cond-mat.mes-hall | we present a solid state implementation of quantum computation which improves previously proposed optically driven schemes our proposal is based on vertical arrays of quantum dots embedded in a mesoporous material which can be fabricated with present technology we study the feasibility of performing quantum computation... | [['we', 'present', 'a', 'solid', 'state', 'implementation', 'of', 'quantum', 'computation', 'which', 'improves', 'previously', 'proposed', 'optically', 'driven', 'schemes', 'our', 'proposal', 'is', 'based', 'on', 'vertical', 'arrays', 'of', 'quantum', 'dots', 'embedded', 'in', 'a', 'mesoporous', 'material', 'which', 'c... | [-0.11147828275676477, 0.1439770551123233, -0.04008330436084758, -0.06150981706291945, 0.02112200646661222, -0.2185855161991309, 0.027613771520555018, 0.430497150326317, -0.22651987490667538, -0.27807099562222987, 0.08811267771313644, -0.22191757513633506, -0.17182841954583472, 0.2355541649232195, -0.030209664347983726... |
709.4136 | X-ray Emission from Planetary Nebulae and their Central Stars: a Status
Report | In the era of Chandra and XMM-Newton, the detection (or nondetection) of
diffuse and/or point-like X-ray sources within planetary nebulae (PNe) yields
important, unique insight into PN shaping processes. Diffuse X-ray sources,
whether due to ``hot bubbles'' or to collimated outflows or jets, allow us to
probe the ene... | astro-ph | in the era of chandra and xmmnewton the detection or nondetection of diffuse andor pointlike xray sources within planetary nebulae pne yields important unique insight into pn shaping processes diffuse xray sources whether due to hot bubbles or to collimated outflows or jets allow us to probe the energetic shocks within... | [['in', 'the', 'era', 'of', 'chandra', 'and', 'xmmnewton', 'the', 'detection', 'or', 'nondetection', 'of', 'diffuse', 'andor', 'pointlike', 'xray', 'sources', 'within', 'planetary', 'nebulae', 'pne', 'yields', 'important', 'unique', 'insight', 'into', 'pn', 'shaping', 'processes', 'diffuse', 'xray', 'sources', 'whether... | [-0.0662847311468795, 0.08807461444754154, -0.09283358297776431, 0.14084940917789937, -0.15033348296768964, -0.06309517855755985, 0.07670268432237208, 0.44822067677974703, -0.20205907768104225, -0.344374310541898, 0.02132650859944988, -0.32727493315935136, -0.008725563080515713, 0.21885244494536893, 0.02834015800151974... |
709.4137 | The relativistic velocity addition law optimizes a forecast gambler's
profit | We extend the projective covariant bookmaker's bets model to the forecasting
gamblers case. The probability of correctness of forecasts shifts probabilities
of branching. The formula for the shift of probabilities leads to the velocity
addition rule of the special theory of relativity. In the absence of
information a... | physics.data-an physics.soc-ph | we extend the projective covariant bookmakers bets model to the forecasting gamblers case the probability of correctness of forecasts shifts probabilities of branching the formula for the shift of probabilities leads to the velocity addition rule of the special theory of relativity in the absence of information about b... | [['we', 'extend', 'the', 'projective', 'covariant', 'bookmakers', 'bets', 'model', 'to', 'the', 'forecasting', 'gamblers', 'case', 'the', 'probability', 'of', 'correctness', 'of', 'forecasts', 'shifts', 'probabilities', 'of', 'branching', 'the', 'formula', 'for', 'the', 'shift', 'of', 'probabilities', 'leads', 'to', 't... | [-0.12046487043300012, 0.0871556524577881, -0.08691689272921893, 0.13606412390870373, -0.0734426295084338, -0.12485511703116278, 0.16628937178616215, 0.29841321733059184, -0.23309475516960507, -0.23405226363590168, 0.05556319710881179, -0.25324659314261927, -0.10168987915911261, 0.14772622413828126, -0.1261775477999641... |
709.4138 | How do the grains slide in fine-grained zirconia polycrystals at high
temperature? | Degradation of mechanical properties of zirconia polycrystals is hardly
discussed in terms of solution-precipitation grain-boundary sliding due to
experimental controversies over imaging of intergranular amorphous phases at
high and room temperatures. Here, the authors applied the techniques of
mechanical spectroscop... | cond-mat.mtrl-sci | degradation of mechanical properties of zirconia polycrystals is hardly discussed in terms of solutionprecipitation grainboundary sliding due to experimental controversies over imaging of intergranular amorphous phases at high and room temperatures here the authors applied the techniques of mechanical spectroscopy and ... | [['degradation', 'of', 'mechanical', 'properties', 'of', 'zirconia', 'polycrystals', 'is', 'hardly', 'discussed', 'in', 'terms', 'of', 'solutionprecipitation', 'grainboundary', 'sliding', 'due', 'to', 'experimental', 'controversies', 'over', 'imaging', 'of', 'intergranular', 'amorphous', 'phases', 'at', 'high', 'and', ... | [-0.06878943130483522, 0.2536730608545066, -0.11898411901704237, -0.10996329581123028, 0.03222995331310028, -0.13636202481118778, 0.07400508085893485, 0.4716356944877143, -0.2364280750682833, -0.29243176821254047, 0.06148234255127974, -0.3636006110658248, -0.12233609574682572, 0.19429869704204156, -0.042862481067833656... |
709.4139 | Serendipitous Chandra X-ray Detection of a Hot Bubble within the
Planetary Nebula NGC 5315 | We report the serendipitous detection of the planetary nebula NGC 5315 by the
Chandra X-ray Observatory. The Chandra imaging spectroscopy results indicate
that the X-rays from this PN, which harbors a Wolf-Rayet (WR) central star,
emanate from a T_X ~ 2.5x10^6 K plasma generated via the same wind-wind
collisions that... | astro-ph | we report the serendipitous detection of the planetary nebula ngc 5315 by the chandra xray observatory the chandra imaging spectroscopy results indicate that the xrays from this pn which harbors a wolfrayet wr central star emanate from a t_x 25x106 k plasma generated via the same windwind collisions that have cleared a... | [['we', 'report', 'the', 'serendipitous', 'detection', 'of', 'the', 'planetary', 'nebula', 'ngc', '5315', 'by', 'the', 'chandra', 'xray', 'observatory', 'the', 'chandra', 'imaging', 'spectroscopy', 'results', 'indicate', 'that', 'the', 'xrays', 'from', 'this', 'pn', 'which', 'harbors', 'a', 'wolfrayet', 'wr', 'central'... | [-0.03027018606448301, 0.11333434779662639, -0.06512890956854742, 0.10275290377781188, -0.10355393752014559, -0.05614278573545897, 0.05021848010579369, 0.46779118827299065, -0.14142851215790295, -0.33032308448302117, 0.038937420764934935, -0.3331986622933887, 0.024701379261616814, 0.2321867171740642, -0.005888844378932... |
709.414 | Fr\"ohlich Polarons from 0D to 3D: Concepts and Recent Developments | I analyse our present understanding of the Froehlich polaron with emphasis on
the response properties, in particular optical absorption.
| cond-mat.mes-hall | i analyse our present understanding of the froehlich polaron with emphasis on the response properties in particular optical absorption | [['i', 'analyse', 'our', 'present', 'understanding', 'of', 'the', 'froehlich', 'polaron', 'with', 'emphasis', 'on', 'the', 'response', 'properties', 'in', 'particular', 'optical', 'absorption']] | [-0.07587378888734077, 0.020628649790428187, -0.03344713857299403, 0.009305219362048726, -0.04258925252054867, -0.10152860848527205, 0.03054949801758324, 0.44906465787636607, -0.15640709215873166, -0.23395744279811256, 0.06320325336051419, -0.2863806701559377, -0.18129309933436544, 0.139908424725658, 0.0221877738245223... |
709.4141 | On representation theory of affine Hecke algebras of type B | Ariki's and Grojnowski's approach to the representation theory of affine
Hecke algebras of type $A$ is applied to type $B$ with unequal parameters to
obtain -- under certain restrictions on the eigenvalues of the lattice
operators -- analogous multiplicity-one results and a classification of
irreducibles with partial... | math.RT | arikis and grojnowskis approach to the representation theory of affine hecke algebras of type a is applied to type b with unequal parameters to obtain under certain restrictions on the eigenvalues of the lattice operators analogous multiplicityone results and a classification of irreducibles with partial branching rule... | [['arikis', 'and', 'grojnowskis', 'approach', 'to', 'the', 'representation', 'theory', 'of', 'affine', 'hecke', 'algebras', 'of', 'type', 'a', 'is', 'applied', 'to', 'type', 'b', 'with', 'unequal', 'parameters', 'to', 'obtain', 'under', 'certain', 'restrictions', 'on', 'the', 'eigenvalues', 'of', 'the', 'lattice', 'ope... | [-0.10346478824154474, 0.06570728368125855, -0.08030849829316139, 0.03378896828973666, -0.12425097521860153, -0.1659885421488434, 0.08691006392939016, 0.30457130309194325, -0.2840418016165495, -0.2017406183714047, 0.1267980592395179, -0.22673853155225515, -0.14582760833203792, 0.18990967797115446, -0.10954648837447166,... |
709.4142 | Colloids dragged through a polymer solution: experiment, theory and
simulation | We present micro-rheological measurments of the drag force on colloids pulled
through a solution of lambda-DNA (used here as a monodisperse model polymer)
with an optical tweezer. The experiments show a violation of the
Stokes-Einstein relation based on the independently measured viscosity of the
DNA solution: the dr... | cond-mat.soft | we present microrheological measurments of the drag force on colloids pulled through a solution of lambdadna used here as a monodisperse model polymer with an optical tweezer the experiments show a violation of the stokeseinstein relation based on the independently measured viscosity of the dna solution the drag force ... | [['we', 'present', 'microrheological', 'measurments', 'of', 'the', 'drag', 'force', 'on', 'colloids', 'pulled', 'through', 'a', 'solution', 'of', 'lambdadna', 'used', 'here', 'as', 'a', 'monodisperse', 'model', 'polymer', 'with', 'an', 'optical', 'tweezer', 'the', 'experiments', 'show', 'a', 'violation', 'of', 'the', '... | [-0.08605391375886479, 0.1462895790909447, -0.1059334002213903, 0.01779176518874298, 0.00014708425831234102, -0.14085127677916004, 0.06205563519915363, 0.33242071692896363, -0.2763524284577089, -0.2702389551086886, 0.027961522184017273, -0.28339389357531425, -0.17312301005153816, 0.19245001042519908, -0.006753878608014... |
709.4143 | A weighted network evolution model based on passenger behavior | This paper presents an evolution model of weighted networks in which the
structural growth and weight dynamics are driven by human behavior, i.e.
passenger route choice behavior. Transportation networks grow due to people's
increasing travel demand and the pattern of growth is determined by their route
choice behavio... | physics.soc-ph physics.data-an | this paper presents an evolution model of weighted networks in which the structural growth and weight dynamics are driven by human behavior ie passenger route choice behavior transportation networks grow due to peoples increasing travel demand and the pattern of growth is determined by their route choice behavior in ai... | [['this', 'paper', 'presents', 'an', 'evolution', 'model', 'of', 'weighted', 'networks', 'in', 'which', 'the', 'structural', 'growth', 'and', 'weight', 'dynamics', 'are', 'driven', 'by', 'human', 'behavior', 'ie', 'passenger', 'route', 'choice', 'behavior', 'transportation', 'networks', 'grow', 'due', 'to', 'peoples', ... | [-0.14059867544551574, 0.14364223452996167, -0.08932663148445402, 0.022905911912744832, -0.06757150829208948, -0.1930899151226164, 0.10009494999812134, 0.3851073302119177, -0.3248356424586175, -0.30150616880762526, 0.02338736730534032, -0.32808263394871406, -0.19418604579649468, 0.11331175491020921, -0.0362085986561445... |
709.4144 | Single crystal growth and anisotropy of CeRuPO | We report on the single crystal growth of the ferromagnetic Kondo lattice
system CeRuPO using a Sn flux method. Magnetic susceptibility and electrical
resistivity measurements indicate strong anisotropy of this structurally
layered compound. They evidence that the magnetic moments order
ferromagnetically along the c-... | cond-mat.str-el cond-mat.mtrl-sci | we report on the single crystal growth of the ferromagnetic kondo lattice system cerupo using a sn flux method magnetic susceptibility and electrical resistivity measurements indicate strong anisotropy of this structurally layered compound they evidence that the magnetic moments order ferromagnetically along the cdirec... | [['we', 'report', 'on', 'the', 'single', 'crystal', 'growth', 'of', 'the', 'ferromagnetic', 'kondo', 'lattice', 'system', 'cerupo', 'using', 'a', 'sn', 'flux', 'method', 'magnetic', 'susceptibility', 'and', 'electrical', 'resistivity', 'measurements', 'indicate', 'strong', 'anisotropy', 'of', 'this', 'structurally', 'l... | [-0.24532848490594789, 0.22682329846396185, 0.03700409115602573, -0.020658992531966288, -0.09889622215160179, -0.11658591952110672, 0.09893345248339505, 0.40667520939565166, -0.28141088036541967, -0.2817948363914058, -0.06945148107713495, -0.34349823102954474, -0.05265852665507245, 0.1243971838219755, 0.149701465582260... |
709.4145 | Stanley decompositions of squarefree modules and Alexander duality | In this paper we study how prime filtrations and squarefree Stanley
decompositions of squarefree modules over the polynomial ring and the exterior
algebra behave with respect to Alexander duality.
| math.AC math.CO | in this paper we study how prime filtrations and squarefree stanley decompositions of squarefree modules over the polynomial ring and the exterior algebra behave with respect to alexander duality | [['in', 'this', 'paper', 'we', 'study', 'how', 'prime', 'filtrations', 'and', 'squarefree', 'stanley', 'decompositions', 'of', 'squarefree', 'modules', 'over', 'the', 'polynomial', 'ring', 'and', 'the', 'exterior', 'algebra', 'behave', 'with', 'respect', 'to', 'alexander', 'duality']] | [-0.22074414237306036, 0.016604665185100044, -0.13483289192462788, 0.03188177652191371, -0.07751006600125854, -0.1693147688076414, -0.16327413900129112, 0.335745214709434, -0.5096374942824758, -0.17035072891980987, 0.07288757246389085, -0.2106477609225388, -0.1743796418966918, 0.10496699524208389, -0.22467682150931195,... |
709.4146 | Signatures of non-monotonic d-wave gap in electron-doped cuprates | We address the issue whether the data on optical conductivity and Raman
scattering in electron-doped cuprates below $T_c$ support the idea that the
$d-$wave gap in these materials is non-monotonic along the Fermi surface. We
calculate the conductivity and Raman intensity for elastic scattering, and find
that a non-mo... | cond-mat.supr-con | we address the issue whether the data on optical conductivity and raman scattering in electrondoped cuprates below t_c support the idea that the dwave gap in these materials is nonmonotonic along the fermi surface we calculate the conductivity and raman intensity for elastic scattering and find that a nonmonotonic gap ... | [['we', 'address', 'the', 'issue', 'whether', 'the', 'data', 'on', 'optical', 'conductivity', 'and', 'raman', 'scattering', 'in', 'electrondoped', 'cuprates', 'below', 't_c', 'support', 'the', 'idea', 'that', 'the', 'dwave', 'gap', 'in', 'these', 'materials', 'is', 'nonmonotonic', 'along', 'the', 'fermi', 'surface', 'w... | [-0.13444228233958158, 0.16163727139193518, -0.07153283911934004, 0.0477884364376269, -0.06836489975287378, -0.1264105195804393, 0.11256773988834193, 0.4562677535334531, -0.28575242247102384, -0.21947714695824852, 0.003795033462251289, -0.41186803558110435, -0.18127822093194043, 0.21187084382753582, 0.03016704505993218... |
709.4147 | Uniqueness of solutions of stochastic differential equations | We consider a d-dimensional stochastic differential equation with additive
noise and a drift coefficient which is assumed only to be a bounded Borel
function. We show that, for almost all choices of the driving Brownian path,
the equation has a unique solution.
| math.PR math.CA | we consider a ddimensional stochastic differential equation with additive noise and a drift coefficient which is assumed only to be a bounded borel function we show that for almost all choices of the driving brownian path the equation has a unique solution | [['we', 'consider', 'a', 'ddimensional', 'stochastic', 'differential', 'equation', 'with', 'additive', 'noise', 'and', 'a', 'drift', 'coefficient', 'which', 'is', 'assumed', 'only', 'to', 'be', 'a', 'bounded', 'borel', 'function', 'we', 'show', 'that', 'for', 'almost', 'all', 'choices', 'of', 'the', 'driving', 'brownia... | [-0.16011860350235588, 0.10454616054803842, -0.10931426073823657, 0.010769986539214318, -0.10839835586514146, -0.15759267826520262, -0.006920279003679752, 0.36038163908579873, -0.3481075671457109, -0.17647504061460495, 0.11220248267359455, -0.29980147825110526, -0.1845812450074369, 0.17125516948068426, -0.0771179202544... |
709.4148 | Quasiclassical generalized Weierstrass representation and dispersionless
DS equation | Quasiclassical generalized Weierstrass representation (GWR) for highly
corrugated surfaces with slow modulation in the four-dimensional Euclidean
space is proposed. Integrable deformations of such surfaces are described by
the dispersionless Davey-Stewartson hierarchy. Quasiclassical GWRs for other
four-dimensional s... | nlin.SI math.DG | quasiclassical generalized weierstrass representation gwr for highly corrugated surfaces with slow modulation in the fourdimensional euclidean space is proposed integrable deformations of such surfaces are described by the dispersionless daveystewartson hierarchy quasiclassical gwrs for other fourdimensional spaces and... | [['quasiclassical', 'generalized', 'weierstrass', 'representation', 'gwr', 'for', 'highly', 'corrugated', 'surfaces', 'with', 'slow', 'modulation', 'in', 'the', 'fourdimensional', 'euclidean', 'space', 'is', 'proposed', 'integrable', 'deformations', 'of', 'such', 'surfaces', 'are', 'described', 'by', 'the', 'dispersion... | [-0.18908491942944916, 0.16590061047395996, -0.005746492238845243, 0.18718981254726735, -0.12547600295308026, -0.20545282985928448, -0.11818428749088632, 0.35751728425452184, -0.27994072363646916, -0.15285165337195925, 0.0806345527336478, -0.2758167879655957, -0.21198056984779445, 0.19895630269203074, -0.11126691807971... |
709.4149 | Wrapped Magnetized Branes: Two Alternative Descriptions? | We discuss two inequivalent ways for describing magnetized D-branes wrapped N
times on a torus T^2. The first one is based on a non-abelian gauge bundle
U(N), while the second one is obtained by means of a Narain T-duality
transformation acting on a theory with non-magnetized branes. We construct in
both descriptions... | hep-th | we discuss two inequivalent ways for describing magnetized dbranes wrapped n times on a torus t2 the first one is based on a nonabelian gauge bundle un while the second one is obtained by means of a narain tduality transformation acting on a theory with nonmagnetized branes we construct in both descriptions the boundar... | [['we', 'discuss', 'two', 'inequivalent', 'ways', 'for', 'describing', 'magnetized', 'dbranes', 'wrapped', 'n', 'times', 'on', 'a', 'torus', 't2', 'the', 'first', 'one', 'is', 'based', 'on', 'a', 'nonabelian', 'gauge', 'bundle', 'un', 'while', 'the', 'second', 'one', 'is', 'obtained', 'by', 'means', 'of', 'a', 'narain'... | [-0.18389813209984587, 0.2024442172515091, -0.07794429663715235, 0.09164450871444234, -0.10068722832895648, -0.1715512355329113, 0.007158524517671027, 0.3470987186066053, -0.15964253025464295, -0.23016885754893, 0.08183001891416863, -0.26102567860186937, -0.126420707287518, 0.13607218626133177, -0.06237271771337209, -0... |
709.415 | Generic behaviours in impact fragmentation | We present a simple numerical model for investigating the general properties
of fragmentation. By use of molecular dynamics simulations, we study the impact
fragmentation of a solid disk of interacting particles with a wall. Regardless
of the particular form of the interaction potential, the fragment size
distributio... | cond-mat.stat-mech | we present a simple numerical model for investigating the general properties of fragmentation by use of molecular dynamics simulations we study the impact fragmentation of a solid disk of interacting particles with a wall regardless of the particular form of the interaction potential the fragment size distribution exhi... | [['we', 'present', 'a', 'simple', 'numerical', 'model', 'for', 'investigating', 'the', 'general', 'properties', 'of', 'fragmentation', 'by', 'use', 'of', 'molecular', 'dynamics', 'simulations', 'we', 'study', 'the', 'impact', 'fragmentation', 'of', 'a', 'solid', 'disk', 'of', 'interacting', 'particles', 'with', 'a', 'w... | [-0.1378723007591465, 0.1430123896425357, -0.14647762969584216, 0.026541956586916517, -0.00187639087288275, -0.06526648433572507, 0.007706145635110479, 0.33395277797185546, -0.23740834515258857, -0.2746321446486289, 0.032899626420186005, -0.2855937569578992, -0.12128931687720403, 0.16200323043025652, 0.0476206863841301... |
709.4151 | Universal description of the rotational-vibrational spectrum of three
particles with zero-range interactions | A comprehensive universal description of the rotational-vibrational spectrum
for two identical particles of mass $m$ and the third particle of the mass
$m_1$ in the zero-range limit of the interaction between different particles is
given for arbitrary values of the mass ratio $m/m_1$ and the total angular
momentum $L... | physics.atom-ph | a comprehensive universal description of the rotationalvibrational spectrum for two identical particles of mass m and the third particle of the mass m_1 in the zerorange limit of the interaction between different particles is given for arbitrary values of the mass ratio mm_1 and the total angular momentum l if the twob... | [['a', 'comprehensive', 'universal', 'description', 'of', 'the', 'rotationalvibrational', 'spectrum', 'for', 'two', 'identical', 'particles', 'of', 'mass', 'm', 'and', 'the', 'third', 'particle', 'of', 'the', 'mass', 'm_1', 'in', 'the', 'zerorange', 'limit', 'of', 'the', 'interaction', 'between', 'different', 'particle... | [-0.1639613665009294, 0.2667704442404007, -0.01599304597249733, 0.053002097340468624, 0.0232534185077364, -0.16783545724793128, 0.03836232895932359, 0.28262659477812996, -0.19954089733741445, -0.3131611632549616, -0.0013688358725074048, -0.3409748060343777, -0.007907808024838281, 0.17423665898539065, 0.0674607385537724... |
709.4152 | Cosmological implications of the KATRIN experiment | The upcoming Karlsruhe Tritium Neutrino (KATRIN) experiment will put
unprecedented constraints on the absolute mass of the electron neutrino,
$\mnue$. In this paper we investigate how this information on $\mnue$ will
affect our constraints on cosmological parameters. We consider two scenarios;
one where $\mnue=0$ (i.... | astro-ph hep-ph | the upcoming karlsruhe tritium neutrino katrin experiment will put unprecedented constraints on the absolute mass of the electron neutrino mnue in this paper we investigate how this information on mnue will affect our constraints on cosmological parameters we consider two scenarios one where mnue0 ie no detection by ka... | [['the', 'upcoming', 'karlsruhe', 'tritium', 'neutrino', 'katrin', 'experiment', 'will', 'put', 'unprecedented', 'constraints', 'on', 'the', 'absolute', 'mass', 'of', 'the', 'electron', 'neutrino', 'mnue', 'in', 'this', 'paper', 'we', 'investigate', 'how', 'this', 'information', 'on', 'mnue', 'will', 'affect', 'our', '... | [-0.0661366515991728, 0.14877323036636697, -0.05517244530485922, 0.12346917544386946, -0.07868005890985218, -0.11661455287399251, 0.04485739966503899, 0.2954545354240396, -0.17504275094173596, -0.3462063158663471, 0.13169795348638605, -0.3254219575921136, -0.04000628819124082, 0.26577645841609226, 0.0025327557402275752... |
709.4153 | Finite Element Formalism for Micromagnetism | The aim of this work is to present the details of the finite element approach
we developed for solving the Landau-Lifschitz-Gilbert equations in order to be
able to treat problems involving complex geometries. There are several
possibilities to solve the complex Landau-Lifschitz-Gilbert equations
numerically. Our met... | cond-mat.other | the aim of this work is to present the details of the finite element approach we developed for solving the landaulifschitzgilbert equations in order to be able to treat problems involving complex geometries there are several possibilities to solve the complex landaulifschitzgilbert equations numerically our method is b... | [['the', 'aim', 'of', 'this', 'work', 'is', 'to', 'present', 'the', 'details', 'of', 'the', 'finite', 'element', 'approach', 'we', 'developed', 'for', 'solving', 'the', 'landaulifschitzgilbert', 'equations', 'in', 'order', 'to', 'be', 'able', 'to', 'treat', 'problems', 'involving', 'complex', 'geometries', 'there', 'ar... | [-0.07891350644255492, 0.04572526806671368, -0.10771611562769867, 0.04588102846392395, -0.09326003284606718, -0.0995897908351048, 0.0038175584898939483, 0.37805253415039386, -0.26988737060534385, -0.27013690792080153, 0.12211427045723465, -0.24975809319070855, -0.13424880326466454, 0.2305067549372106, -0.02245882257146... |
709.4154 | Lower bounds on the canonical height associated to the morphism \phi(z)=
z^d+c | Certain lower bounds are obtained on the canonical height associated to the
morphism $\phi(z)=z^d+c$.
| math.NT math.DS | certain lower bounds are obtained on the canonical height associated to the morphism phizzdc | [['certain', 'lower', 'bounds', 'are', 'obtained', 'on', 'the', 'canonical', 'height', 'associated', 'to', 'the', 'morphism', 'phizzdc']] | [-0.17717178294864985, 0.13125402594988161, -0.03715497011748644, 0.18557836172672418, -0.08247763835466825, -0.1298074652082645, 0.015089809894561768, 0.3249126420571254, -0.378586009144783, -0.2994693082112532, 0.08578768472831982, -0.22379776620520994, -0.0540787553271422, 0.3587947218463971, -0.1404368503449055, 0.... |
709.4155 | Photonuclear reactions of actinide and pre-actinide nuclei at
intermediate energies | Photonuclear reaction is described with an approach based on the
quasideuteron nuclear photoabsorption model followed by the process of
competition between light particle evaporation and fission for the excited
nucleus. Thus fission process is considered as a decay mode. The
evaporation-fission process of the compoun... | nucl-th physics.chem-ph | photonuclear reaction is described with an approach based on the quasideuteron nuclear photoabsorption model followed by the process of competition between light particle evaporation and fission for the excited nucleus thus fission process is considered as a decay mode the evaporationfission process of the compound nuc... | [['photonuclear', 'reaction', 'is', 'described', 'with', 'an', 'approach', 'based', 'on', 'the', 'quasideuteron', 'nuclear', 'photoabsorption', 'model', 'followed', 'by', 'the', 'process', 'of', 'competition', 'between', 'light', 'particle', 'evaporation', 'and', 'fission', 'for', 'the', 'excited', 'nucleus', 'thus', '... | [0.03272437713811266, 0.21271295394077153, -0.06005556631087112, 0.15553907573590908, 0.09637972158899905, -0.06667901687400385, 0.046838113415955764, 0.39292703129229, -0.17605518004532567, -0.29285995103418827, -0.07388732078977571, -0.3673224131057619, 0.07212871482565267, 0.18986423483374146, 0.10347886295744875, 0... |
709.4156 | Raman imaging of doping domains in graphene on SiO2 | We present spatially resolved Raman images of the G and 2D lines of
single-layer graphene flakes. The spatial fluctuations of G and 2D lines are
correlated and are thus shown to be affiliated with local doping domains. We
investigate the position of the 2D line -- the most significant Raman peak to
identify single-la... | cond-mat.mtrl-sci | we present spatially resolved raman images of the g and 2d lines of singlelayer graphene flakes the spatial fluctuations of g and 2d lines are correlated and are thus shown to be affiliated with local doping domains we investigate the position of the 2d line the most significant raman peak to identify singlelayer graph... | [['we', 'present', 'spatially', 'resolved', 'raman', 'images', 'of', 'the', 'g', 'and', '2d', 'lines', 'of', 'singlelayer', 'graphene', 'flakes', 'the', 'spatial', 'fluctuations', 'of', 'g', 'and', '2d', 'lines', 'are', 'correlated', 'and', 'are', 'thus', 'shown', 'to', 'be', 'affiliated', 'with', 'local', 'doping', 'd... | [-0.13409289013890718, 0.08382759918218233, 0.007622301116708882, -0.02671588770660364, -0.030269401342307857, -0.18646817057093312, 0.07283515385005715, 0.4840208430243425, -0.22941709825988427, -0.2794840756235144, 0.009115498562050937, -0.33412316407669673, -0.11086783852920798, 0.15533451935947942, -0.0012861480474... |
709.4157 | A combinatorial and field theoretic path to quantum gravity: the new
challenges of group field theory | Group field theories are a new type of field theories over group manifolds
and a generalization of matrix models, that have recently attracted much
interest in quantum gravity research. They represent a development of and a
possible link between different approaches such as loop quantum gravity and
simplicial quantum... | hep-th gr-qc | group field theories are a new type of field theories over group manifolds and a generalization of matrix models that have recently attracted much interest in quantum gravity research they represent a development of and a possible link between different approaches such as loop quantum gravity and simplicial quantum gra... | [['group', 'field', 'theories', 'are', 'a', 'new', 'type', 'of', 'field', 'theories', 'over', 'group', 'manifolds', 'and', 'a', 'generalization', 'of', 'matrix', 'models', 'that', 'have', 'recently', 'attracted', 'much', 'interest', 'in', 'quantum', 'gravity', 'research', 'they', 'represent', 'a', 'development', 'of', ... | [-0.09698297481236795, 0.1372194487350778, -0.1198167862718577, 0.10029564149406545, -0.1645290340491376, -0.21950037375215317, 0.018956916245560233, 0.3648725091940263, -0.23070959637330457, -0.3049538675286285, 0.1084031633160251, -0.24792669017052094, -0.20219189904701823, 0.2166289643404985, -0.11063424807430787, 0... |
709.4158 | Infrared spectroscopic diagnostics for Active Galactic Nuclei | Infrared spectroscopy in the mid- and far-infrared provides powerful
diagnostics for studying the emission regions in active galaxies. The large
variety of ionic fine structure lines can probe gas conditions in a variety of
physical conditions, from highly ionized gas excited by photons originated by
black hole accre... | astro-ph | infrared spectroscopy in the mid and farinfrared provides powerful diagnostics for studying the emission regions in active galaxies the large variety of ionic fine structure lines can probe gas conditions in a variety of physical conditions from highly ionized gas excited by photons originated by black hole accretion t... | [['infrared', 'spectroscopy', 'in', 'the', 'mid', 'and', 'farinfrared', 'provides', 'powerful', 'diagnostics', 'for', 'studying', 'the', 'emission', 'regions', 'in', 'active', 'galaxies', 'the', 'large', 'variety', 'of', 'ionic', 'fine', 'structure', 'lines', 'can', 'probe', 'gas', 'conditions', 'in', 'a', 'variety', '... | [-0.04450973168359664, 0.12152655801868864, -0.03466691152823175, 0.10848608023562231, -0.07511503634372761, -0.07452605669881993, 0.04123356817174495, 0.46519863662188465, -0.14892873122293201, -0.3187600328089519, 0.05648024397633206, -0.29233846132591457, -0.010466446773212705, 0.2044818517347069, 0.0186045810374899... |
709.4159 | Torques on Spheroidal Silicate Grains Exposed to Anisotropic
Interstellar Radiation Fields | Radiative torques, due to the absorption and scattering of starlight, are
thought to play a major role in the alignment of grains with the interstellar
magnetic field. The absorption of radiation also gives rise to recoil torques,
associated with the photoelectric effect and photodesorption. The recoil
torques are mu... | astro-ph | radiative torques due to the absorption and scattering of starlight are thought to play a major role in the alignment of grains with the interstellar magnetic field the absorption of radiation also gives rise to recoil torques associated with the photoelectric effect and photodesorption the recoil torques are much more... | [['radiative', 'torques', 'due', 'to', 'the', 'absorption', 'and', 'scattering', 'of', 'starlight', 'are', 'thought', 'to', 'play', 'a', 'major', 'role', 'in', 'the', 'alignment', 'of', 'grains', 'with', 'the', 'interstellar', 'magnetic', 'field', 'the', 'absorption', 'of', 'radiation', 'also', 'gives', 'rise', 'to', '... | [-0.05112073096137315, 0.13078122719969243, -0.04425048179388659, 0.05992539621226183, -0.10462630793335848, -0.05347161680740649, -0.0010628567702353818, 0.4113089453990329, -0.24733184534443975, -0.35586477254759774, 0.01274283702185454, -0.2848807579059511, -0.06571474865920944, 0.22597956234806102, -0.0087223958944... |
709.416 | Origin of the abundance patterns in Galactic globular clusters:
constraints on dynamical and chemical properties of globular clusters | Aims. We analyse the effects of a first generation of fast rotating massive
stars on the dynamical and chemical properties of globular clusters. Methods.
We use stellar models of fast rotating massive stars, losing mass through a
slow mechanical equatorial winds to produce material rich in H-burning
products. We prop... | astro-ph | aims we analyse the effects of a first generation of fast rotating massive stars on the dynamical and chemical properties of globular clusters methods we use stellar models of fast rotating massive stars losing mass through a slow mechanical equatorial winds to produce material rich in hburning products we propose that... | [['aims', 'we', 'analyse', 'the', 'effects', 'of', 'a', 'first', 'generation', 'of', 'fast', 'rotating', 'massive', 'stars', 'on', 'the', 'dynamical', 'and', 'chemical', 'properties', 'of', 'globular', 'clusters', 'methods', 'we', 'use', 'stellar', 'models', 'of', 'fast', 'rotating', 'massive', 'stars', 'losing', 'mass... | [-0.062435651508142634, 0.16464183106905397, -0.07265196961501764, 0.11001841470597601, -0.06612296347235758, -0.04517924406123662, 0.08184394358997107, 0.4072616946839451, -0.14443655013943696, -0.37899372266956316, -0.007004158981175892, -0.2781676609364867, -0.02406442345803756, 0.19692831069885477, -0.0597792630338... |
709.4161 | Galactic Rotation Parameters from Data on Open Star Clusters | Currently available data on the field of velocities Vr, Vl, Vb for open star
clusters are used to perform a kinematic analysis of various samples that
differ by heliocentric distance, age, and membership in individual structures
(the Orion, Carina--Sagittarius, and Perseus arms). Based on 375 clusters
located within ... | astro-ph | currently available data on the field of velocities vr vl vb for open star clusters are used to perform a kinematic analysis of various samples that differ by heliocentric distance age and membership in individual structures the orion carinasagittarius and perseus arms based on 375 clusters located within 5 kpc of the ... | [['currently', 'available', 'data', 'on', 'the', 'field', 'of', 'velocities', 'vr', 'vl', 'vb', 'for', 'open', 'star', 'clusters', 'are', 'used', 'to', 'perform', 'a', 'kinematic', 'analysis', 'of', 'various', 'samples', 'that', 'differ', 'by', 'heliocentric', 'distance', 'age', 'and', 'membership', 'in', 'individual',... | [-0.04922442783860771, 0.11789762083757317, -0.07819303026663652, 0.05078658720485005, -0.08656225612448563, -0.05092153433367955, 0.06878729805873074, 0.44094987793491697, -0.2210307304647461, -0.3698735240636007, 0.040086297329871054, -0.24600167424068786, 0.02348748471160674, 0.1917638737205328, -0.01825176490984751... |
709.4162 | Benchmark density functional theory calculations for nano-scale
conductance | We present a set of benchmark calculations for the Kohn-Sham elastic
transmission function of five representative single-molecule junctions. The
transmission functions are calculated using two different density functional
theory (DFT) methods, namely an ultrasoft pseudopotential plane wave code in
combination with ma... | cond-mat.mes-hall | we present a set of benchmark calculations for the kohnsham elastic transmission function of five representative singlemolecule junctions the transmission functions are calculated using two different density functional theory dft methods namely an ultrasoft pseudopotential plane wave code in combination with maximally ... | [['we', 'present', 'a', 'set', 'of', 'benchmark', 'calculations', 'for', 'the', 'kohnsham', 'elastic', 'transmission', 'function', 'of', 'five', 'representative', 'singlemolecule', 'junctions', 'the', 'transmission', 'functions', 'are', 'calculated', 'using', 'two', 'different', 'density', 'functional', 'theory', 'dft'... | [-0.13060056572661086, 0.0715838760072022, -0.08217764181661145, 0.0756315640860619, 0.022990535331635382, -0.09908093060467311, 0.05538253185737932, 0.41909559825502285, -0.2395634848336361, -0.2452633342698967, 0.018122688775024504, -0.28920647724390885, -0.12299816954458842, 0.16650236340192742, 0.06479936579523755,... |
709.4163 | On statistical mechanics in noncommutative spaces | We study the formulation of quantum statistical mechanics in noncommutative
spaces. We construct microcanonical and canonical ensemble theory in
noncommutative spaces. We consider for illustration some basic and important
examples in the framework of noncommutative statistical mechanics : (i). An
electron in a magnet... | hep-th | we study the formulation of quantum statistical mechanics in noncommutative spaces we construct microcanonical and canonical ensemble theory in noncommutative spaces we consider for illustration some basic and important examples in the framework of noncommutative statistical mechanics i an electron in a magnetic field ... | [['we', 'study', 'the', 'formulation', 'of', 'quantum', 'statistical', 'mechanics', 'in', 'noncommutative', 'spaces', 'we', 'construct', 'microcanonical', 'and', 'canonical', 'ensemble', 'theory', 'in', 'noncommutative', 'spaces', 'we', 'consider', 'for', 'illustration', 'some', 'basic', 'and', 'important', 'examples',... | [-0.044483742535313855, 0.14122979487027415, -0.07778171593755749, 0.18124289055620985, 0.012363112115833377, -0.16527734761725046, -0.03547980875633324, 0.34129155709940406, -0.26294529212048345, -0.21914875703597708, 0.026370724203713638, -0.24964293824242695, -0.18848588473130284, 0.17657578554644715, -0.12312397430... |
709.4164 | Compound-specific isotope analysis | The isotopic composition, for example, 14C/12C, 13C/12C, 2H/1H, 15N/14N and
18O/16O, of the elements of matter is heterogeneous. It is ruled by physical,
chemical and biological mechanisms. Isotopes can be employed to follow the fate
of mineral and organic compounds during biogeochemical transformations. The
determin... | q-bio.BM | the isotopic composition for example 14c12c 13c12c 2h1h 15n14n and 18o16o of the elements of matter is heterogeneous it is ruled by physical chemical and biological mechanisms isotopes can be employed to follow the fate of mineral and organic compounds during biogeochemical transformations the determination of the isot... | [['the', 'isotopic', 'composition', 'for', 'example', '14c12c', '13c12c', '2h1h', '15n14n', 'and', '18o16o', 'of', 'the', 'elements', 'of', 'matter', 'is', 'heterogeneous', 'it', 'is', 'ruled', 'by', 'physical', 'chemical', 'and', 'biological', 'mechanisms', 'isotopes', 'can', 'be', 'employed', 'to', 'follow', 'the', '... | [-0.05961563422105613, 0.1858445543845275, -0.035999003810132234, 0.01832077745863327, 0.011159719258497378, -0.07064732361947541, 0.06324325604014, 0.3671297827422355, -0.2248564524806838, -0.31241420307402723, 0.06759627342051043, -0.268620887804216, -0.13798114186795676, 0.17155717276201576, -0.03154267740345239, 0.... |
709.4165 | Observation of B^+ Meson Decays to a1(1260)^+ K^0 and B^0 to a1(1260)^-
K^+ | We present branching fraction measurements of the decays B^{+} ->
a1(1260)^{+} K^{0} and B^{0} to a1(1260)^{-} K^{+} with a1(1260)^{+} -> pi^{-}
pi^{+} pi^{+}. The data sample corresponds to 383 million B B-bar pairs
produced in e^{+}e^{-} annihilation through the Y(4S) resonance. We measure the
products of the branc... | hep-ex | we present branching fraction measurements of the decays b a11260 k0 and b0 to a11260 k with a11260 pi pi pi the data sample corresponds to 383 million b bbar pairs produced in ee annihilation through the y4s resonance we measure the products of the branching fractions bb a11260 k0ba11260 pi pi pi 174 25 22 106 bb0 a11... | [['we', 'present', 'branching', 'fraction', 'measurements', 'of', 'the', 'decays', 'b', 'a11260', 'k0', 'and', 'b0', 'to', 'a11260', 'k', 'with', 'a11260', 'pi', 'pi', 'pi', 'the', 'data', 'sample', 'corresponds', 'to', '383', 'million', 'b', 'bbar', 'pairs', 'produced', 'in', 'ee', 'annihilation', 'through', 'the', 'y... | [-0.17237825712354313, 0.2613965155636912, -0.061717451004291414, 0.034011161533154304, -0.013026581676576728, -0.07409121843695801, 0.24109982813693462, 0.2751686012282247, -0.20301509845841637, -0.2684304215094095, -0.08000827422590866, -0.5128046139193478, 0.11354881733335474, 0.09233376045300755, 0.0985402260376240... |
709.4166 | Timescale effect estimation in time-series studies of air pollution and
health: A Singular Spectrum Analysis approach | A wealth of epidemiological data suggests an association between
mortality/morbidity from pulmonary and cardiovascular adverse events and air
pollution, but uncertainty remains as to the extent implied by those
associations although the abundance of the data. In this paper we describe an
SSA (Singular Spectrum Analys... | stat.AP | a wealth of epidemiological data suggests an association between mortalitymorbidity from pulmonary and cardiovascular adverse events and air pollution but uncertainty remains as to the extent implied by those associations although the abundance of the data in this paper we describe an ssa singular spectrum analysis bas... | [['a', 'wealth', 'of', 'epidemiological', 'data', 'suggests', 'an', 'association', 'between', 'mortalitymorbidity', 'from', 'pulmonary', 'and', 'cardiovascular', 'adverse', 'events', 'and', 'air', 'pollution', 'but', 'uncertainty', 'remains', 'as', 'to', 'the', 'extent', 'implied', 'by', 'those', 'associations', 'altho... | [-0.06251209097130125, 0.07611089487541713, -0.10428641274767486, 0.11259181697632333, -0.03872144112461492, -0.038480468295318516, 0.08466205076486068, 0.33744902270600985, -0.23023793750295513, -0.32164515839203406, 0.14234406273370903, -0.33938485317324335, -0.13900842963178692, 0.19126937185463153, -0.1336052500912... |
709.4167 | Automatic generation of vertices for the Schroedinger functional | We present a multiplication algorithm to recursively construct vertices for
the Schroedinger functional in the abelian background field case. The algorithm
is suited for automatic perturbative calculations with a variety of actions. As
first applications, we derive ratios of the lambda parameters between the
lattice ... | hep-lat | we present a multiplication algorithm to recursively construct vertices for the schroedinger functional in the abelian background field case the algorithm is suited for automatic perturbative calculations with a variety of actions as first applications we derive ratios of the lambda parameters between the lattice schem... | [['we', 'present', 'a', 'multiplication', 'algorithm', 'to', 'recursively', 'construct', 'vertices', 'for', 'the', 'schroedinger', 'functional', 'in', 'the', 'abelian', 'background', 'field', 'case', 'the', 'algorithm', 'is', 'suited', 'for', 'automatic', 'perturbative', 'calculations', 'with', 'a', 'variety', 'of', 'a... | [-0.15136629898289714, 0.1422623427042478, -0.06799202796095345, 0.056031342032896, -0.05667414138965969, -0.14592673931317993, 0.08138253986599701, 0.41281342039568514, -0.19029296033049026, -0.29291716331168066, 0.05717963484098215, -0.23826485459344268, -0.1380840131270263, 0.16980965739068918, 0.020470842165000076,... |
709.4168 | Two-phonon assisted exciton spin relaxation due to exchange interaction
in spherical quantum dots | Spin relaxation in undoped quasi-spherical CdS quantum dots at zero magnetic
fields is investigated using time- and polarization-resolved transient
absorption measurements. Unlike in previous studies of these systems, the
measured signals were corrected for spin-insensitive contributions to the
exciton bleaching dyna... | cond-mat.mes-hall | spin relaxation in undoped quasispherical cds quantum dots at zero magnetic fields is investigated using time and polarizationresolved transient absorption measurements unlike in previous studies of these systems the measured signals were corrected for spininsensitive contributions to the exciton bleaching dynamics all... | [['spin', 'relaxation', 'in', 'undoped', 'quasispherical', 'cds', 'quantum', 'dots', 'at', 'zero', 'magnetic', 'fields', 'is', 'investigated', 'using', 'time', 'and', 'polarizationresolved', 'transient', 'absorption', 'measurements', 'unlike', 'in', 'previous', 'studies', 'of', 'these', 'systems', 'the', 'measured', 's... | [-0.11486001207570856, 0.2119781665359672, -0.04551940678259901, 0.04444671647506766, 0.016861512830170493, -0.15431678240420296, 0.042033380237019934, 0.4451231547010442, -0.2358174500016806, -0.266635352584611, -0.015823943074792624, -0.3167264910026764, -0.04869257144940396, 0.20332186112257963, 0.07401847369037569,... |
709.4169 | Exorcizing the Landau Ghost in Non Commutative Quantum Field Theory | We show that the simplest non commutative renormalizable field theory, the
$\phi^4$ model on four dimensional Moyal space with harmonic potential is
asymptotically safe to all orders in perturbation theory
| hep-th | we show that the simplest non commutative renormalizable field theory the phi4 model on four dimensional moyal space with harmonic potential is asymptotically safe to all orders in perturbation theory | [['we', 'show', 'that', 'the', 'simplest', 'non', 'commutative', 'renormalizable', 'field', 'theory', 'the', 'phi4', 'model', 'on', 'four', 'dimensional', 'moyal', 'space', 'with', 'harmonic', 'potential', 'is', 'asymptotically', 'safe', 'to', 'all', 'orders', 'in', 'perturbation', 'theory']] | [-0.1570421090039114, 0.16769413053213308, -0.049118486046791074, 0.11064084140040602, -0.0528040803813686, -0.18480580411851405, -0.07060653558777025, 0.33199336112787325, -0.19504574462771415, -0.16480124748001496, 0.04368277784669772, -0.30221354827905694, -0.23608585993448894, 0.1437782915852343, -0.042695700253049... |
709.417 | Subleading properties of the QCD flux-tube in 3-d lattice gauge theory | We study the continuum limit of the string-like behaviour of flux tubes
formed between static quarks and anti-quarks in three dimensional SU(2) lattice
gauge theory. We compare our simulation data with the predictions of both
effective string models as well as perturbation theory. On the string side we
obtain clear e... | hep-lat | we study the continuum limit of the stringlike behaviour of flux tubes formed between static quarks and antiquarks in three dimensional su2 lattice gauge theory we compare our simulation data with the predictions of both effective string models as well as perturbation theory on the string side we obtain clear evidence ... | [['we', 'study', 'the', 'continuum', 'limit', 'of', 'the', 'stringlike', 'behaviour', 'of', 'flux', 'tubes', 'formed', 'between', 'static', 'quarks', 'and', 'antiquarks', 'in', 'three', 'dimensional', 'su2', 'lattice', 'gauge', 'theory', 'we', 'compare', 'our', 'simulation', 'data', 'with', 'the', 'predictions', 'of', ... | [-0.07604529014436387, 0.13725364033415025, -0.1291745279078223, 0.17409182206077986, -0.023062634700517944, -0.12544313655039216, 0.06121728861579249, 0.33211316630056426, -0.18674000864628382, -0.29487225464975636, 0.062337577423206024, -0.3241037467040685, -0.1280683388198851, 0.12281296629176922, 0.0105434805585243... |
709.4171 | Global existence for a kinetic model of chemotaxis via dispersion and
Strichartz estimates | We investigate further the existence of solutions to kinetic models of
chemotaxis. These are nonlinear transport-scattering equations with a quadratic
nonlinearity which have been used to describe the motion of bacteria since the
80's when experimental observations have shown they move by a series of 'run
and tumble'... | math.AP | we investigate further the existence of solutions to kinetic models of chemotaxis these are nonlinear transportscattering equations with a quadratic nonlinearity which have been used to describe the motion of bacteria since the 80s when experimental observations have shown they move by a series of run and tumble the ex... | [['we', 'investigate', 'further', 'the', 'existence', 'of', 'solutions', 'to', 'kinetic', 'models', 'of', 'chemotaxis', 'these', 'are', 'nonlinear', 'transportscattering', 'equations', 'with', 'a', 'quadratic', 'nonlinearity', 'which', 'have', 'been', 'used', 'to', 'describe', 'the', 'motion', 'of', 'bacteria', 'since'... | [-0.06835229264705799, 0.03936052550253568, -0.06865734535762492, -0.014498849397675847, -0.10496951874152086, -0.11578980775084347, 0.012992494710488245, 0.32948514653424565, -0.20758052171047037, -0.3646619627320701, 0.11600641245005296, -0.27564416958621757, -0.16852058118606425, 0.20410719286198453, -0.090437629852... |
709.4172 | Spin-polarized Current-induced Instability in Spin-Valve with
Antiferromagnetic Layer | In the framework of phenomenological model we consider dynamics of a
compensated collinear antiferromagnet (AFM) in the presence of spin-polarised
current. The model is based on the assumption that AFM spins are localised and
spin torque is transferred to each magnetic sublattice independently. It is
shown that in AF... | cond-mat.mtrl-sci | in the framework of phenomenological model we consider dynamics of a compensated collinear antiferromagnet afm in the presence of spinpolarised current the model is based on the assumption that afm spins are localised and spin torque is transferred to each magnetic sublattice independently it is shown that in afm spin ... | [['in', 'the', 'framework', 'of', 'phenomenological', 'model', 'we', 'consider', 'dynamics', 'of', 'a', 'compensated', 'collinear', 'antiferromagnet', 'afm', 'in', 'the', 'presence', 'of', 'spinpolarised', 'current', 'the', 'model', 'is', 'based', 'on', 'the', 'assumption', 'that', 'afm', 'spins', 'are', 'localised', '... | [-0.20525960510059696, 0.24105016842522486, -0.05830163450683562, 0.003925249540028448, -0.07031230533457532, -0.133063513861627, 0.025692653737734168, 0.38747437847588134, -0.3045160776783465, -0.26156981893796094, 0.015391182475153128, -0.29531650871456583, -0.06017018986773221, 0.1679775712640994, 0.0719451605180772... |
709.4173 | An Alternative Form of the Functional Equation for Riemann's Zeta
Function | In this paper we present a simple method for deriving an alternative form of
the functional equation for Riemann's Zeta function. The connections between
some functional equations obtained implicitly by Leonhard Euler in his work
"Remarques sur un beau rapport entre les series des puissances tant directes
que recipro... | math.HO math.NT | in this paper we present a simple method for deriving an alternative form of the functional equation for riemanns zeta function the connections between some functional equations obtained implicitly by leonhard euler in his work remarques sur un beau rapport entre les series des puissances tant directes que reciproques ... | [['in', 'this', 'paper', 'we', 'present', 'a', 'simple', 'method', 'for', 'deriving', 'an', 'alternative', 'form', 'of', 'the', 'functional', 'equation', 'for', 'riemanns', 'zeta', 'function', 'the', 'connections', 'between', 'some', 'functional', 'equations', 'obtained', 'implicitly', 'by', 'leonhard', 'euler', 'in', ... | [-0.1390502208214776, -0.02285955677673388, -0.2016990011100445, 0.1052370301443724, -0.1290667279656127, -0.059232406600035335, -0.0644737301943742, 0.2333096509917819, -0.24272175937732213, -0.28696615499722067, 0.05827860456274561, -0.2702617231070211, -0.23898907316227755, 0.19451814259222724, -0.11007604997180272,... |
709.4174 | Angular Distributions of B -> K ll Decays | We model-independently analyze the angular distributions of B -> K ll decays,
l = e, mu, for low dilepton mass using QCD factorization. Besides the decay
rate, we study the forward-backward asymmetry A_FB^l and a further observable,
F_H^l, which gives rise to a flat term in the angular distribution. We find
that in t... | hep-ph | we modelindependently analyze the angular distributions of b k ll decays l e mu for low dilepton mass using qcd factorization besides the decay rate we study the forwardbackward asymmetry a_fbl and a further observable f_hl which gives rise to a flat term in the angular distribution we find that in the standard model f... | [['we', 'modelindependently', 'analyze', 'the', 'angular', 'distributions', 'of', 'b', 'k', 'll', 'decays', 'l', 'e', 'mu', 'for', 'low', 'dilepton', 'mass', 'using', 'qcd', 'factorization', 'besides', 'the', 'decay', 'rate', 'we', 'study', 'the', 'forwardbackward', 'asymmetry', 'a_fbl', 'and', 'a', 'further', 'observa... | [-0.12425375320530256, 0.19369382126081625, -0.043828352955273715, 0.0883512768815479, -0.03782947913231789, -0.17676256454577394, 0.08998177505137472, 0.2964871586392643, -0.2324451077959989, -0.2764871937129416, 0.0015344120600113257, -0.3180085164419892, 0.006165320676115185, 0.14175547741118377, 0.06923128639423924... |
709.4175 | Fast Fourier Transforms for the Rook Monoid | We define the notion of the Fourier transform for the rook monoid (also
called the symmetric inverse semigroup) and provide two efficient
divide-and-conquer algorithms (fast Fourier transforms, or FFTs) for computing
it. This paper marks the first extension of group FFTs to non-group semigroups.
| math.RT math.NA | we define the notion of the fourier transform for the rook monoid also called the symmetric inverse semigroup and provide two efficient divideandconquer algorithms fast fourier transforms or ffts for computing it this paper marks the first extension of group ffts to nongroup semigroups | [['we', 'define', 'the', 'notion', 'of', 'the', 'fourier', 'transform', 'for', 'the', 'rook', 'monoid', 'also', 'called', 'the', 'symmetric', 'inverse', 'semigroup', 'and', 'provide', 'two', 'efficient', 'divideandconquer', 'algorithms', 'fast', 'fourier', 'transforms', 'or', 'ffts', 'for', 'computing', 'it', 'this', '... | [-0.07997381310401992, 0.07920010682110759, -0.1452298995784738, 0.13142319051919252, -0.19162795497951182, -0.09120503889227455, 0.030080327756216073, 0.4013719101521102, -0.41213870370252564, -0.18926853212443265, 0.18155535665044392, -0.2423552542670884, -0.19547414016084408, 0.23754483663519335, -0.0483535946061072... |
709.4176 | Angular momentum quantization from Planck's energy quantization | We present in this work a pedagogical way of quantizing the atomic orbit for
the hydrogen's atom model proposed by Bohr without using his hypothesis of
angular momentum quantization. In contrast to the usual treatment for the
orbital quantization, we show that using energy conservation, correspondence
principle and P... | quant-ph | we present in this work a pedagogical way of quantizing the atomic orbit for the hydrogens atom model proposed by bohr without using his hypothesis of angular momentum quantization in contrast to the usual treatment for the orbital quantization we show that using energy conservation correspondence principle and planks ... | [['we', 'present', 'in', 'this', 'work', 'a', 'pedagogical', 'way', 'of', 'quantizing', 'the', 'atomic', 'orbit', 'for', 'the', 'hydrogens', 'atom', 'model', 'proposed', 'by', 'bohr', 'without', 'using', 'his', 'hypothesis', 'of', 'angular', 'momentum', 'quantization', 'in', 'contrast', 'to', 'the', 'usual', 'treatment... | [-0.10960728687826883, 0.1221527225464921, -0.12010910509464641, 0.08542423577455338, -0.05755025729762785, -0.10832290296358141, 0.09194075554312969, 0.32299572187052533, -0.25513561719774525, -0.32781651170190534, -0.02208316601657619, -0.20999505705284802, -0.1006234772221157, 0.14441810440709532, -0.110248936453100... |
709.4177 | Detailed Spectral Modeling of a 3-D Pulsating Reverse Detonation Model:
Too Much Nickel | We calculate detailed NLTE synthetic spectra of a Pulsating Reverse
Detonation (PRD) model, a novel explosion mechanism for Type Ia supernovae.
While the hydro models are calculated in 3-D, the spectra use an angle averaged
hydro model and thus some of the 3-D details are lost, but the overall average
should be a g... | astro-ph | we calculate detailed nlte synthetic spectra of a pulsating reverse detonation prd model a novel explosion mechanism for type ia supernovae while the hydro models are calculated in 3d the spectra use an angle averaged hydro model and thus some of the 3d details are lost but the overall average should be a good represen... | [['we', 'calculate', 'detailed', 'nlte', 'synthetic', 'spectra', 'of', 'a', 'pulsating', 'reverse', 'detonation', 'prd', 'model', 'a', 'novel', 'explosion', 'mechanism', 'for', 'type', 'ia', 'supernovae', 'while', 'the', 'hydro', 'models', 'are', 'calculated', 'in', '3d', 'the', 'spectra', 'use', 'an', 'angle', 'averag... | [-0.023792304193529373, 0.06644459269912495, -0.04956526487635878, 0.12779625331362088, -0.10224786439719491, -0.1902599511987482, 0.0649468791217376, 0.44788882023631, -0.19495888943291412, -0.29554926079387467, 0.0664193836828837, -0.31464903954034434, -0.08188902480312837, 0.1785874934389423, -0.06534628746796023, -... |
709.4178 | Threshold phenomena on product spaces: BKKKL revisited (once more) | We revisit the work of Bourgain, Kahn, Kalai, Katznelson and Linial (1992) --
referred to as ``BKKKL'' in the title -- about influences on Boolean functions
in order to give a precise statement of threshold phenomenon on the product
space $\{1,..., r\}^\NN$, generalizing one of the main results of a paper by
Talagran... | math.PR | we revisit the work of bourgain kahn kalai katznelson and linial 1992 referred to as bkkkl in the title about influences on boolean functions in order to give a precise statement of threshold phenomenon on the product space 1 rnn generalizing one of the main results of a paper by talagrand 1994 | [['we', 'revisit', 'the', 'work', 'of', 'bourgain', 'kahn', 'kalai', 'katznelson', 'and', 'linial', '1992', 'referred', 'to', 'as', 'bkkkl', 'in', 'the', 'title', 'about', 'influences', 'on', 'boolean', 'functions', 'in', 'order', 'to', 'give', 'a', 'precise', 'statement', 'of', 'threshold', 'phenomenon', 'on', 'the', ... | [-0.08927288107000865, 0.034813408027940355, -0.061364267845279895, 0.10559108262308516, -0.08387333589892548, -0.06376106383350606, 0.08369420037398903, 0.25671994714782786, -0.24745562780075347, -0.30083692424858993, 0.10066461499081925, -0.2552305822296498, -0.18824239728900677, 0.1838847346191939, -0.21384785965514... |
709.4179 | Relaxational dynamics in 3D randomly diluted Ising models | We study the purely relaxational dynamics (model A) at criticality in
three-dimensional disordered Ising systems whose static critical behaviour
belongs to the randomly diluted Ising universality class. We consider the
site-diluted and bond-diluted Ising models, and the +- J Ising model along the
paramagnetic-ferroma... | cond-mat.dis-nn cond-mat.stat-mech | we study the purely relaxational dynamics model a at criticality in threedimensional disordered ising systems whose static critical behaviour belongs to the randomly diluted ising universality class we consider the sitediluted and bonddiluted ising models and the j ising model along the paramagneticferromagnetic transi... | [['we', 'study', 'the', 'purely', 'relaxational', 'dynamics', 'model', 'a', 'at', 'criticality', 'in', 'threedimensional', 'disordered', 'ising', 'systems', 'whose', 'static', 'critical', 'behaviour', 'belongs', 'to', 'the', 'randomly', 'diluted', 'ising', 'universality', 'class', 'we', 'consider', 'the', 'sitediluted'... | [-0.14089295694536372, 0.15874097805845383, -0.11515497966746163, 0.06441979082840744, 0.03212761319144459, -0.18394789180900084, 0.05328862874260422, 0.3171725860206274, -0.22270418200982597, -0.2283954254306126, 0.0781692081126072, -0.3009629913310452, -0.14549531086834955, 0.1334876472488182, 0.09982728855911552, 0.... |
709.418 | Local superfluid densities probed via current-induced superconducting
phase gradients | We have developed a superconducting phase gradiometer consisting of two
parallel DNA-templated nanowires connecting two thin-film leads. We have ramped
the cross current flowing perpendicular to the nanowires, and observed
oscillations in the lead-to-lead resistance due to cross-current-induced phase
differences. By ... | cond-mat.supr-con | we have developed a superconducting phase gradiometer consisting of two parallel dnatemplated nanowires connecting two thinfilm leads we have ramped the cross current flowing perpendicular to the nanowires and observed oscillations in the leadtolead resistance due to crosscurrentinduced phase differences by using this ... | [['we', 'have', 'developed', 'a', 'superconducting', 'phase', 'gradiometer', 'consisting', 'of', 'two', 'parallel', 'dnatemplated', 'nanowires', 'connecting', 'two', 'thinfilm', 'leads', 'we', 'have', 'ramped', 'the', 'cross', 'current', 'flowing', 'perpendicular', 'to', 'the', 'nanowires', 'and', 'observed', 'oscillat... | [-0.2116994715520534, 0.22614937052602382, -0.05655824341650667, -0.023952014911545163, -0.008933754434445124, -0.09038200611569758, 0.04539293488059407, 0.3758678784187155, -0.23778941164371267, -0.322174489155583, -0.0006702169896392472, -0.2871298923574645, -0.08960348469119561, 0.19077504706440557, 0.00939866497941... |
709.4181 | Violation of the Wiedemann-Franz Law in a Single-Electron Transistor | We study the influence of Coulomb interaction on the thermoelectric transport
coefficients for a metallic single-electron transistor. By performing a
perturbation expansion up to second order in the tunnel-barrier conductance, we
include sequential and cotunneling processes as well as quantum fluctuations
that renorm... | cond-mat.mes-hall | we study the influence of coulomb interaction on the thermoelectric transport coefficients for a metallic singleelectron transistor by performing a perturbation expansion up to second order in the tunnelbarrier conductance we include sequential and cotunneling processes as well as quantum fluctuations that renormalize ... | [['we', 'study', 'the', 'influence', 'of', 'coulomb', 'interaction', 'on', 'the', 'thermoelectric', 'transport', 'coefficients', 'for', 'a', 'metallic', 'singleelectron', 'transistor', 'by', 'performing', 'a', 'perturbation', 'expansion', 'up', 'to', 'second', 'order', 'in', 'the', 'tunnelbarrier', 'conductance', 'we',... | [-0.2056093912997699, 0.16052496858932538, -0.0468126650097126, 0.06049629458488817, 0.0008701641692165682, -0.1830463844965747, 0.13407344145556674, 0.3252192835640558, -0.2667954091795106, -0.28961535079523604, -0.04048403854571045, -0.33211739109630917, -0.1574399981578376, 0.20953420733914097, 0.03382758774170454, ... |
709.4182 | Giant magnetoresistance and extraordinary magnetoresistance in
inhomogeneous semiconducting DyNiBi | The semiconducting half-Heulser compound DyNiBi shows a negative giant
magnetoresistance (GMR) below 200 K. Except for a weak deviation, this
magnetoresistance scales roughly with the square of the magnetization in the
paramagnetic state, and is related to the metal-insulator transition. At low
temperature, a positiv... | cond-mat.mtrl-sci | the semiconducting halfheulser compound dynibi shows a negative giant magnetoresistance gmr below 200 k except for a weak deviation this magnetoresistance scales roughly with the square of the magnetization in the paramagnetic state and is related to the metalinsulator transition at low temperature a positive magnetore... | [['the', 'semiconducting', 'halfheulser', 'compound', 'dynibi', 'shows', 'a', 'negative', 'giant', 'magnetoresistance', 'gmr', 'below', '200', 'k', 'except', 'for', 'a', 'weak', 'deviation', 'this', 'magnetoresistance', 'scales', 'roughly', 'with', 'the', 'square', 'of', 'the', 'magnetization', 'in', 'the', 'paramagnet... | [-0.2006068975984383, 0.24846324540063072, -0.014344544698998554, 0.00750848888106811, -0.04963512139380979, -0.16196949921770773, 0.06776286794025618, 0.32314030156095525, -0.2508295475602595, -0.33508677487331096, 0.011540091497503888, -0.35566621212594546, -0.08634738825650802, 0.17889151487972088, 0.051142081465405... |
709.4183 | Role of defects and disorder in the half-metallic full-Heusler compounds | Half-metallic ferromagnets and especially the full-Heusler alloys containing
Co are at the center of scientific research due to their potential applications
in spintronics. For realistic devices it is important to control accurately the
creation of defects in these alloys. We review some of our late results on the
ro... | cond-mat.mtrl-sci | halfmetallic ferromagnets and especially the fullheusler alloys containing co are at the center of scientific research due to their potential applications in spintronics for realistic devices it is important to control accurately the creation of defects in these alloys we review some of our late results on the role of ... | [['halfmetallic', 'ferromagnets', 'and', 'especially', 'the', 'fullheusler', 'alloys', 'containing', 'co', 'are', 'at', 'the', 'center', 'of', 'scientific', 'research', 'due', 'to', 'their', 'potential', 'applications', 'in', 'spintronics', 'for', 'realistic', 'devices', 'it', 'is', 'important', 'to', 'control', 'accur... | [-0.08777487478312104, 0.13102905719913543, 0.052567834835499525, 0.053662593646906315, 0.002854748027399182, -0.1358199059292674, 0.09890336557291449, 0.45248530931770803, -0.21139045026898384, -0.26830496080964805, 0.01794516657292843, -0.39069844472780824, -0.15727312313392758, 0.16500989337265493, -0.01875318819098... |
709.4184 | Observation of Ds1(2536)+ -> D+pi-K+ and angular decomposition of
Ds1(2536)+ -> D*+K0S | Using 462/fb of e+e- annihilation data recorded by the Belle detector, we
report the first observation of the decay Ds1(2536)+ -> D+pi-K+. The ratio of
branching fractions B(Ds1+ -> D+pi-K+)/B(Ds1+ -> D*+K0) is measured to be
(3.27+-0.18+-0.37)%. We also study the angular distributions in the Ds1(2536)+
-> D*+K0S dec... | hep-ex | using 462fb of ee annihilation data recorded by the belle detector we report the first observation of the decay ds12536 dpik the ratio of branching fractions bds1 dpikbds1 dk0 is measured to be 327018037 we also study the angular distributions in the ds12536 dk0s decay and measure the ratio of d and swave amplitudes th... | [['using', '462fb', 'of', 'ee', 'annihilation', 'data', 'recorded', 'by', 'the', 'belle', 'detector', 'we', 'report', 'the', 'first', 'observation', 'of', 'the', 'decay', 'ds12536', 'dpik', 'the', 'ratio', 'of', 'branching', 'fractions', 'bds1', 'dpikbds1', 'dk0', 'is', 'measured', 'to', 'be', '327018037', 'we', 'also'... | [-0.1476883388445059, 0.17958739337821802, -0.09823549468593117, 0.055296289826449206, -0.01881216502372633, -0.07937850047458421, 0.06338133368837207, 0.30859645351506115, -0.19537821784615517, -0.25255499657635627, -0.0014933038261931454, -0.36439105789912374, 0.014102300122510968, 0.13815871838954064, 0.123064664960... |
709.4185 | On local equivalence problem of spacetimes with two orthogonally
transitive commuting Killing fields | Considered is the problem of local equivalence of generic four-dimensional
metrics possessing two commuting and orthogonally transitive Killing vector
fields. A sufficient set of eight differential invariants is explicitly
constructed, among them four of first order and four of second order in terms
of metric coeffic... | math-ph math.MP | considered is the problem of local equivalence of generic fourdimensional metrics possessing two commuting and orthogonally transitive killing vector fields a sufficient set of eight differential invariants is explicitly constructed among them four of first order and four of second order in terms of metric coefficients... | [['considered', 'is', 'the', 'problem', 'of', 'local', 'equivalence', 'of', 'generic', 'fourdimensional', 'metrics', 'possessing', 'two', 'commuting', 'and', 'orthogonally', 'transitive', 'killing', 'vector', 'fields', 'a', 'sufficient', 'set', 'of', 'eight', 'differential', 'invariants', 'is', 'explicitly', 'construct... | [-0.22410288632943712, 0.10300940762932316, 0.011094802155576903, 0.06543472404832598, -0.07873943350117268, -0.15129205493802397, -0.06870261235323188, 0.3088504948396364, -0.22138779905046627, -0.2813655816275498, 0.08463800076248751, -0.3055122806851206, -0.17819417136368051, 0.13843964248221238, -0.0229514132350169... |
709.4186 | The Accretion Flows and Evolution of Magnetic Cataclysmic Variables | We have used a model of magnetic accretion to investigate the accretion flows
of magnetic cataclysmic variables. Numerical simulations demonstrate that four
types of flow are possible: discs, streams, rings and propellers. The
fundamental observable determining the accretion flow, for a given mass ratio,
is the spin-... | astro-ph | we have used a model of magnetic accretion to investigate the accretion flows of magnetic cataclysmic variables numerical simulations demonstrate that four types of flow are possible discs streams rings and propellers the fundamental observable determining the accretion flow for a given mass ratio is the spintoorbital ... | [['we', 'have', 'used', 'a', 'model', 'of', 'magnetic', 'accretion', 'to', 'investigate', 'the', 'accretion', 'flows', 'of', 'magnetic', 'cataclysmic', 'variables', 'numerical', 'simulations', 'demonstrate', 'that', 'four', 'types', 'of', 'flow', 'are', 'possible', 'discs', 'streams', 'rings', 'and', 'propellers', 'the... | [-0.17463566534031458, 0.21296079194224957, -0.05449524958169571, 0.06270406403389105, -0.0328014597536013, -0.08431804474201743, 0.013540903446954434, 0.39992673361889, -0.2453738845522619, -0.37092963039416377, 0.10737730720817733, -0.26808261420107254, -0.02961424444112237, 0.19811144502104813, -0.02773633141381045,... |
709.4187 | A Semiclassical String Description of Wilson Loop with Local Operators | We discuss a semiclassical string description to circular Wilson loops
without/with local operator insertions. By considering a semiclassical
approximation of type IIB string theory on AdS_5 X S^5 around the corresponding
classical solutions, quadratic actions with respect to fluctuations are
computed. Then the dual ... | hep-th | we discuss a semiclassical string description to circular wilson loops withoutwith local operator insertions by considering a semiclassical approximation of type iib string theory on ads_5 x s5 around the corresponding classical solutions quadratic actions with respect to fluctuations are computed then the dual corresp... | [['we', 'discuss', 'a', 'semiclassical', 'string', 'description', 'to', 'circular', 'wilson', 'loops', 'withoutwith', 'local', 'operator', 'insertions', 'by', 'considering', 'a', 'semiclassical', 'approximation', 'of', 'type', 'iib', 'string', 'theory', 'on', 'ads_5', 'x', 's5', 'around', 'the', 'corresponding', 'class... | [-0.1666603561089788, 0.14258951040230589, -0.07029406481888145, 0.15151461106466335, -0.046453726908010945, -0.12961097622367865, 0.0366131560214045, 0.3007108360632426, -0.21049874178263256, -0.19456213465390546, 0.09076863140702092, -0.32287668278958237, -0.13885278637624449, 0.13094894566004062, -0.0857736537000164... |
709.4188 | Charge imbalance and Josephson effects in superconductor-normal metal
mesoscopic structures | We consider a $SBS$ Josephson junction the superconducting electrodes $S$ of
which are in contact with normal metal reservoirs ($B$ means a barrier). For
temperatures near $T_{c}$ we calculate an effective critical current $%
I_{c}^{\ast}$ and the resistance of the system at the currents $I<$ $%
I_{c}^{\ast}$ and $I>... | cond-mat.supr-con cond-mat.mes-hall | we consider a sbs josephson junction the superconducting electrodes s of which are in contact with normal metal reservoirs b means a barrier for temperatures near t_c we calculate an effective critical current i_cast and the resistance of the system at the currents i i_cast and ii_cast it is found that the charge imbal... | [['we', 'consider', 'a', 'sbs', 'josephson', 'junction', 'the', 'superconducting', 'electrodes', 's', 'of', 'which', 'are', 'in', 'contact', 'with', 'normal', 'metal', 'reservoirs', 'b', 'means', 'a', 'barrier', 'for', 'temperatures', 'near', 't_c', 'we', 'calculate', 'an', 'effective', 'critical', 'current', 'i_cast',... | [-0.202970535952581, 0.18649920136570136, -0.02361519016190677, 0.010340573669772743, 0.014104904766243539, -0.16319774449374036, 0.09285951624655067, 0.3035108134101488, -0.2603339040835731, -0.26287850830703974, -0.0021099157518045487, -0.3377607614782296, -0.08090608944813109, 0.18889792974560374, 0.0153893064738153... |
709.4189 | Strong homotopy inner product of an A-infinity algebra | We introduce a strong homotopy notion of a cyclic symmetric inner product of
an A-infinity algebra and prove a characterization theorem in the formalism of
the infinity inner products by Tradler. We also show that it is equivalent to
the notion of a non-constant symplectic structure on the corresponding formal
non-co... | math.AT math.SG | we introduce a strong homotopy notion of a cyclic symmetric inner product of an ainfinity algebra and prove a characterization theorem in the formalism of the infinity inner products by tradler we also show that it is equivalent to the notion of a nonconstant symplectic structure on the corresponding formal noncommutat... | [['we', 'introduce', 'a', 'strong', 'homotopy', 'notion', 'of', 'a', 'cyclic', 'symmetric', 'inner', 'product', 'of', 'an', 'ainfinity', 'algebra', 'and', 'prove', 'a', 'characterization', 'theorem', 'in', 'the', 'formalism', 'of', 'the', 'infinity', 'inner', 'products', 'by', 'tradler', 'we', 'also', 'show', 'that', '... | [-0.17771933886200883, 0.06343822037211624, -0.11004623593112757, 0.08312382909934968, -0.10428822325910767, -0.12569288807639548, -0.028747120698870615, 0.3547539821674311, -0.4038349782539055, -0.1843976431991905, 0.0635527829561101, -0.15676972867791042, -0.2128100481349975, 0.15083336910817685, -0.1794191734800332,... |
709.419 | Local to Global Compatibility on the Eigencurve (l not equal p) | We generalise Coleman's construction of Hecke operators to define an action
of GL_2(Q_l) on the space of finite slope overconvergent p-adic modular forms
(l not equal p). In this way we associate to any C_p-valued point on the tame
level N Coleman-Mazur eigencurve an admissible smooth representation of
GL_2(Q_l) exte... | math.NT | we generalise colemans construction of hecke operators to define an action of gl_2q_l on the space of finite slope overconvergent padic modular forms l not equal p in this way we associate to any c_pvalued point on the tame level n colemanmazur eigencurve an admissible smooth representation of gl_2q_l extending the cla... | [['we', 'generalise', 'colemans', 'construction', 'of', 'hecke', 'operators', 'to', 'define', 'an', 'action', 'of', 'gl_2q_l', 'on', 'the', 'space', 'of', 'finite', 'slope', 'overconvergent', 'padic', 'modular', 'forms', 'l', 'not', 'equal', 'p', 'in', 'this', 'way', 'we', 'associate', 'to', 'any', 'c_pvalued', 'point'... | [-0.1806902411427894, 0.046981690789746094, -0.23069407095246744, 0.06834926564536034, -0.13738793230377047, -0.11222607930469122, 0.02723179521357141, 0.28273419465687943, -0.349210844852212, -0.19470095761949424, 0.01762423680799945, -0.22572440189513854, -0.16205332891606702, 0.1906692966387221, -0.181082696250708, ... |
709.4191 | Two Sides of Spin Concept | The notion of the spin is shown to have two constituents, as exemplified by
the spin of the electron. The first one is related to the form of the wave
equation and determines the fermion or boson particle type. This implies the
spin taking strictly half-integer or integer number. The second side of spin
manifestation... | quant-ph | the notion of the spin is shown to have two constituents as exemplified by the spin of the electron the first one is related to the form of the wave equation and determines the fermion or boson particle type this implies the spin taking strictly halfinteger or integer number the second side of spin manifestation is rel... | [['the', 'notion', 'of', 'the', 'spin', 'is', 'shown', 'to', 'have', 'two', 'constituents', 'as', 'exemplified', 'by', 'the', 'spin', 'of', 'the', 'electron', 'the', 'first', 'one', 'is', 'related', 'to', 'the', 'form', 'of', 'the', 'wave', 'equation', 'and', 'determines', 'the', 'fermion', 'or', 'boson', 'particle', '... | [-0.17171167652249214, 0.22573518465936143, -0.039739875208950885, 0.06029829996228016, -0.07034914147706055, -0.09290505691593431, -0.035903075524560256, 0.28895863735764893, -0.27243068166401074, -0.28218648388333945, 0.0646499301289188, -0.2649262779918702, -0.12228551759566787, 0.178039337998084, 0.0354261758190620... |
709.4192 | Parametrization of the Driven Betatron Oscillation | An AC dipole is a magnet which produces a sinusoidally oscillating dipole
field and excites coherent transverse beam motion in a synchrotron. By
observing this coherent motion, the optical parameters can be directly measured
at the beam position monitor locations. The driven oscillation induced by an AC
dipole will g... | physics.acc-ph | an ac dipole is a magnet which produces a sinusoidally oscillating dipole field and excites coherent transverse beam motion in a synchrotron by observing this coherent motion the optical parameters can be directly measured at the beam position monitor locations the driven oscillation induced by an ac dipole will genera... | [['an', 'ac', 'dipole', 'is', 'a', 'magnet', 'which', 'produces', 'a', 'sinusoidally', 'oscillating', 'dipole', 'field', 'and', 'excites', 'coherent', 'transverse', 'beam', 'motion', 'in', 'a', 'synchrotron', 'by', 'observing', 'this', 'coherent', 'motion', 'the', 'optical', 'parameters', 'can', 'be', 'directly', 'meas... | [-0.12484950723224565, 0.19214761606341008, -0.09023523683120546, 0.04203124920482208, -0.10365753485576103, -0.10953852583801275, 0.008209594765580015, 0.39648949605853934, -0.2739227070718219, -0.28309675588419564, 0.02768174825775388, -0.24551623498187644, -0.04639686653145442, 0.25893173811614123, -0.04437403109316... |
709.4193 | Exact Vacuum Energy of Orbifold Lattice Theories | We investigate the orbifold lattice theories constructed from supersymmetric
Yang-Mills matrix theories (mother theories) with four and eight supercharges.
We show that the vacuum energy of these theories does not receive any quantum
correction perturbatively.
| hep-lat hep-th | we investigate the orbifold lattice theories constructed from supersymmetric yangmills matrix theories mother theories with four and eight supercharges we show that the vacuum energy of these theories does not receive any quantum correction perturbatively | [['we', 'investigate', 'the', 'orbifold', 'lattice', 'theories', 'constructed', 'from', 'supersymmetric', 'yangmills', 'matrix', 'theories', 'mother', 'theories', 'with', 'four', 'and', 'eight', 'supercharges', 'we', 'show', 'that', 'the', 'vacuum', 'energy', 'of', 'these', 'theories', 'does', 'not', 'receive', 'any', ... | [-0.1336509468300002, 0.23978604591850725, -0.07286496272842799, 0.1194977581501007, -0.01623429866241557, -0.23760392208184514, -0.046832804794290236, 0.3313355984432357, -0.1156892718481166, -0.2490030096045562, 0.04925342840142548, -0.3148749340325594, -0.20437522530555724, 0.03150763884186745, -0.05187185848397868,... |
709.4194 | Microscopic theory of the Casimir force at thermal equilibrium:
large-separation asymptotics | We present an entirely microscopic calculation of the Casimir force $f(d)$
between two metallic plates in the limit of large separation $d$. The models of
metals consist of mobile quantum charges in thermal equilibrium with the photon
field at positive temperature $T$. Fluctuations of all degrees of freedom,
matter a... | quant-ph | we present an entirely microscopic calculation of the casimir force fd between two metallic plates in the limit of large separation d the models of metals consist of mobile quantum charges in thermal equilibrium with the photon field at positive temperature t fluctuations of all degrees of freedom matter and field are ... | [['we', 'present', 'an', 'entirely', 'microscopic', 'calculation', 'of', 'the', 'casimir', 'force', 'fd', 'between', 'two', 'metallic', 'plates', 'in', 'the', 'limit', 'of', 'large', 'separation', 'd', 'the', 'models', 'of', 'metals', 'consist', 'of', 'mobile', 'quantum', 'charges', 'in', 'thermal', 'equilibrium', 'wit... | [-0.17025736914100972, 0.17031500656186394, -0.09510996495814514, 0.04571378360163759, -0.03599341108047432, -0.14283082480401252, 0.058677504205137884, 0.3099245320525811, -0.20928723963372636, -0.29164674495713727, -0.0045320391143446395, -0.2874699051731802, -0.10167514898630818, 0.13181313795344482, -0.003615425543... |
709.4195 | Monte Carlo studies of the VERITAS array of Cherenkov telescopes | VERITAS is a system of four imaging Cherenkov telescopes located at the Fred
Lawrence Whipple Observatory in southern Arizona. We present here results of
detailed Monte Carlo simulations of the array response to extensive air
showers. Cherenkov image and shower parameter distributions are calculated and
show good agr... | astro-ph | veritas is a system of four imaging cherenkov telescopes located at the fred lawrence whipple observatory in southern arizona we present here results of detailed monte carlo simulations of the array response to extensive air showers cherenkov image and shower parameter distributions are calculated and show good agreeme... | [['veritas', 'is', 'a', 'system', 'of', 'four', 'imaging', 'cherenkov', 'telescopes', 'located', 'at', 'the', 'fred', 'lawrence', 'whipple', 'observatory', 'in', 'southern', 'arizona', 'we', 'present', 'here', 'results', 'of', 'detailed', 'monte', 'carlo', 'simulations', 'of', 'the', 'array', 'response', 'to', 'extensi... | [-0.08172439167772667, 0.17186231126881116, -0.06496827434297771, 0.1427842091295808, -0.029200545594757123, -0.049690302243576415, -0.008727857552003115, 0.4541859620761487, -0.16434428600534315, -0.4382399399351749, 0.07892844064964823, -0.3612037501823638, 0.007778956205584109, 0.23943786500322242, 0.036862309866269... |
709.4196 | Tensor Meson Production in Proton-Proton Collisions from the Color Glass
Condensate | We compute the inclusive cross-section of $f_{2}$ tensor mesons production in
proton-proton collisions at high-energy. We use an effective theory inspired
from the tensor meson dominance hypothesis that couples gluons to $f_{2}$
mesons. We compute the differential cross-section in the
$k_{\perp}$-factorization and in... | hep-ph | we compute the inclusive crosssection of f_2 tensor mesons production in protonproton collisions at highenergy we use an effective theory inspired from the tensor meson dominance hypothesis that couples gluons to f_2 mesons we compute the differential crosssection in the k_perpfactorization and in the color glass conde... | [['we', 'compute', 'the', 'inclusive', 'crosssection', 'of', 'f_2', 'tensor', 'mesons', 'production', 'in', 'protonproton', 'collisions', 'at', 'highenergy', 'we', 'use', 'an', 'effective', 'theory', 'inspired', 'from', 'the', 'tensor', 'meson', 'dominance', 'hypothesis', 'that', 'couples', 'gluons', 'to', 'f_2', 'meso... | [-0.054878436472013736, 0.2190719063641578, -0.18552588874438, 0.17662084507258627, -0.034056873483474824, -0.06979820248896926, -0.04797902477123024, 0.37935408861240716, -0.2216427644208363, -0.19877697240326156, -0.07452025169108822, -0.3235879233468649, -0.04553935026723973, 0.09850218129859677, 0.06191488377777045... |
709.4197 | Search for supernova-produced 60Fe in a marine sediment | An 60Fe peak in a deep-sea FeMn crust has been interpreted as due to the
signature left by the ejecta of a supernova explosion close to the solar system
2.8 +/- 0.4 Myr ago [Knie et al., Phys. Rev. Lett. 93, 171103 (2004)]. To
confirm this interpretation with better time resolution and obtain a more
direct flux estim... | astro-ph | an 60fe peak in a deepsea femn crust has been interpreted as due to the signature left by the ejecta of a supernova explosion close to the solar system 28 04 myr ago knie et al phys rev lett 93 171103 2004 to confirm this interpretation with better time resolution and obtain a more direct flux estimate we measured 60fe... | [['an', '60fe', 'peak', 'in', 'a', 'deepsea', 'femn', 'crust', 'has', 'been', 'interpreted', 'as', 'due', 'to', 'the', 'signature', 'left', 'by', 'the', 'ejecta', 'of', 'a', 'supernova', 'explosion', 'close', 'to', 'the', 'solar', 'system', '28', '04', 'myr', 'ago', 'knie', 'et', 'al', 'phys', 'rev', 'lett', '93', '171... | [-0.008762019824084396, 0.1232661577435535, -0.03134547671428523, 0.0767549698581346, -0.024504830344365194, -0.004794432289110353, 0.12052213489257085, 0.35186910214654815, -0.18282279525346196, -0.38978365681564003, 0.03266838250251917, -0.2755031972281778, -0.05208166994326838, 0.2007177154569385, -0.110274715850559... |
709.4198 | Quantized Detector Networks: A review of recent developments | QDN (quantized detector networks) is a description of quantum processes in
which the principal focus is on observers and their apparatus, rather than on
states of SUOs (systems under observation). It is a realization of Heisenberg's
original instrumentalist approach to quantum physics and can deal with time
dependent... | quant-ph | qdn quantized detector networks is a description of quantum processes in which the principal focus is on observers and their apparatus rather than on states of suos systems under observation it is a realization of heisenbergs original instrumentalist approach to quantum physics and can deal with time dependent apparatu... | [['qdn', 'quantized', 'detector', 'networks', 'is', 'a', 'description', 'of', 'quantum', 'processes', 'in', 'which', 'the', 'principal', 'focus', 'is', 'on', 'observers', 'and', 'their', 'apparatus', 'rather', 'than', 'on', 'states', 'of', 'suos', 'systems', 'under', 'observation', 'it', 'is', 'a', 'realization', 'of',... | [-0.12976111234589058, 0.1844316265122457, -0.12170997959646311, 0.09954509612395089, -0.06966746665368026, -0.2370460624256256, -0.02203240812099962, 0.33289369122675533, -0.24199711578919297, -0.29624099904163315, 0.03538734937002036, -0.28378505292348566, -0.1473541931841861, 0.23715205134887418, -0.0932989398522874... |
709.4199 | Isotope effect on superconductivity in Josephson coupled stripes in
underdoped cuprates | Inelastic neutron scattering data for YBaCuO as well as for LaSrCuO indicate
incommensurate neutron scattering peaks with incommensuration $\delta(x)$ away
from the $(\pi,\pi)$ point. $T_c(x)$ can be replotted as a linear function of
the incommensuration for these materials. This linear relation implies that the
cons... | cond-mat.str-el cond-mat.supr-con | inelastic neutron scattering data for ybacuo as well as for lasrcuo indicate incommensurate neutron scattering peaks with incommensuration deltax away from the pipi point t_cx can be replotted as a linear function of the incommensuration for these materials this linear relation implies that the constant that relates th... | [['inelastic', 'neutron', 'scattering', 'data', 'for', 'ybacuo', 'as', 'well', 'as', 'for', 'lasrcuo', 'indicate', 'incommensurate', 'neutron', 'scattering', 'peaks', 'with', 'incommensuration', 'deltax', 'away', 'from', 'the', 'pipi', 'point', 't_cx', 'can', 'be', 'replotted', 'as', 'a', 'linear', 'function', 'of', 't... | [-0.126366234045325, 0.21362213488216336, -0.041617562251456214, 0.0465869323802692, -0.04089023057516729, -0.14080873944102168, 0.10221967274845292, 0.357746090616148, -0.2937443858453993, -0.24232567025811513, -0.006534044182660176, -0.3592807153896617, -0.08907306881088527, 0.17883744640033583, 0.007833459574696904,... |
709.42 | Copy Number Variants and Segmental Duplications Show Different Formation
Signatures | In addition to variation in terms of single nucleotide polymorphisms (SNPs),
whole regions ranging from several kilobases up to a megabase in length differ
in copy number among individuals. These differences are referred to as Copy
Number Variants (CNVs) and extensive mapping of these is underway. Recent
studies have... | q-bio.GN q-bio.QM | in addition to variation in terms of single nucleotide polymorphisms snps whole regions ranging from several kilobases up to a megabase in length differ in copy number among individuals these differences are referred to as copy number variants cnvs and extensive mapping of these is underway recent studies have highligh... | [['in', 'addition', 'to', 'variation', 'in', 'terms', 'of', 'single', 'nucleotide', 'polymorphisms', 'snps', 'whole', 'regions', 'ranging', 'from', 'several', 'kilobases', 'up', 'to', 'a', 'megabase', 'in', 'length', 'differ', 'in', 'copy', 'number', 'among', 'individuals', 'these', 'differences', 'are', 'referred', 't... | [-0.10397452830276903, 0.15902297763105092, -0.02682084937095492, 0.09497997643460797, -0.021076818772276202, -0.14546121948496288, 0.06676286027340533, 0.4384260535401653, -0.22301808943326074, -0.31694464230602004, 0.06355328577516164, -0.3225914408554203, -0.1691495824056948, 0.14992082575260993, -0.0739302947894752... |
709.4201 | Consequences of the Production of Very Massive Magnetically Charged
Leptons Early in the Universe and Their Decays to a New Set of Extremely
Massive Neutrinos | We examine the production and decay of extremely heavy magnetically charged
leptons, (tau_g and mu_g), to their own very heavy mu_g and e_g plus their own
new species of neutrinos, nu_g and nubar_g, at some time early in the universe
which could be present in space and, attracted gravitationally towards and
passing t... | hep-ph | we examine the production and decay of extremely heavy magnetically charged leptons tau_g and mu_g to their own very heavy mu_g and e_g plus their own new species of neutrinos nu_g and nubar_g at some time early in the universe which could be present in space and attracted gravitationally towards and passing through as... | [['we', 'examine', 'the', 'production', 'and', 'decay', 'of', 'extremely', 'heavy', 'magnetically', 'charged', 'leptons', 'tau_g', 'and', 'mu_g', 'to', 'their', 'own', 'very', 'heavy', 'mu_g', 'and', 'e_g', 'plus', 'their', 'own', 'new', 'species', 'of', 'neutrinos', 'nu_g', 'and', 'nubar_g', 'at', 'some', 'time', 'ear... | [-0.10161839792337478, 0.270097464257642, -0.038464035352252506, 0.10154672023536784, -0.04117470414618428, -0.11953065899106559, 0.050927763362676744, 0.3511161839777834, -0.23713687350554916, -0.33844293065871417, 0.047394549258293985, -0.3227300096742725, 0.015048243919010745, 0.16502992233020788, 0.0074705997164702... |
709.4202 | SUSY Multi-Step Unification without Doublet-Triplet Splitting | Matter-Higgs unification in string-inspired supersymmetric Grand Unified
Theories predicts the existence of colored states in the Higgs multiplets and
calls for two extra generations of Higgs-like fields ('unhiggses'). If these
states are present near the TeV scale, gauge-coupling unification points to the
existence ... | hep-ph | matterhiggs unification in stringinspired supersymmetric grand unified theories predicts the existence of colored states in the higgs multiplets and calls for two extra generations of higgslike fields unhiggses if these states are present near the tev scale gaugecoupling unification points to the existence of two disti... | [['matterhiggs', 'unification', 'in', 'stringinspired', 'supersymmetric', 'grand', 'unified', 'theories', 'predicts', 'the', 'existence', 'of', 'colored', 'states', 'in', 'the', 'higgs', 'multiplets', 'and', 'calls', 'for', 'two', 'extra', 'generations', 'of', 'higgslike', 'fields', 'unhiggses', 'if', 'these', 'states'... | [-0.14563654721197156, 0.3418685958476595, -0.036837578471750024, 0.22381024648978684, -0.09555336008262304, -0.2131580692483112, -0.028944761194806132, 0.2872572419880372, -0.20631663442796302, -0.35840073434842956, 0.02618515811757081, -0.22076617521751257, 0.009144887379888032, 0.05616523930802941, 0.023456139458964... |
709.4203 | Profile of Two-Higgs-Doublet-Model Parameter Space | We review recent work on constraining the parameter space of the
Two-Higgs-Doublet Model by theoretical and experimental results. Some
characteristics of the model, in particular the distribution of masses in the
surviving parameter space, are discussed.
| hep-ph | we review recent work on constraining the parameter space of the twohiggsdoublet model by theoretical and experimental results some characteristics of the model in particular the distribution of masses in the surviving parameter space are discussed | [['we', 'review', 'recent', 'work', 'on', 'constraining', 'the', 'parameter', 'space', 'of', 'the', 'twohiggsdoublet', 'model', 'by', 'theoretical', 'and', 'experimental', 'results', 'some', 'characteristics', 'of', 'the', 'model', 'in', 'particular', 'the', 'distribution', 'of', 'masses', 'in', 'the', 'surviving', 'pa... | [-0.09082251254262196, 0.14396346421239692, -0.011356923806791505, 0.05444327617685, -0.08202351717692283, -0.05575402426378181, 0.05211178751455413, 0.355322369063894, -0.17489030862796223, -0.3098554592579603, 0.0874704525146323, -0.26481229892104036, -0.12803849378704196, 0.2068278972033618, -0.027448121820473008, 0... |
709.4204 | On stable constant mean curvature surfaces in S2 X R and H2 X R | We study stable compact constant mean curvature surfaces in the product
spaces S2 X R and H2 X R and in some other Riemannian 3-manifolds.
| math.DG | we study stable compact constant mean curvature surfaces in the product spaces s2 x r and h2 x r and in some other riemannian 3manifolds | [['we', 'study', 'stable', 'compact', 'constant', 'mean', 'curvature', 'surfaces', 'in', 'the', 'product', 'spaces', 's2', 'x', 'r', 'and', 'h2', 'x', 'r', 'and', 'in', 'some', 'other', 'riemannian', '3manifolds']] | [-0.2640007733553648, 0.09286223035305738, -0.019818768128752707, 0.10939537815749645, -0.025666477084159853, -0.20866890035569668, -0.06002649642527103, 0.48111016988754274, -0.2621067676693201, -0.16239616110920907, 0.1560933341179043, -0.29253930315375326, -0.07170891474466771, 0.15499788301065565, -0.16530314467847... |
709.4205 | Comment on: Competing Interactions, the Renormalization Group, and the
Isotropic-Nematic Phase Transition, by D. Barci and D. Stariolo, Phys. Rev.
Lett. 98, 200604 (2007) | In a recent PRL Barci and Stariolo (BS) generalized the well known Brazovskii
model to include an additional rotationally invariant quartic interaction and
study this model in two dimensions (2d). Depending on the parameters of the
model, BS find two transitions: a first order isotropic-lamellar (striped) or a
second... | cond-mat.stat-mech cond-mat.soft cond-mat.str-el | in a recent prl barci and stariolo bs generalized the well known brazovskii model to include an additional rotationally invariant quartic interaction and study this model in two dimensions 2d depending on the parameters of the model bs find two transitions a first order isotropiclamellar striped or a second order isotr... | [['in', 'a', 'recent', 'prl', 'barci', 'and', 'stariolo', 'bs', 'generalized', 'the', 'well', 'known', 'brazovskii', 'model', 'to', 'include', 'an', 'additional', 'rotationally', 'invariant', 'quartic', 'interaction', 'and', 'study', 'this', 'model', 'in', 'two', 'dimensions', '2d', 'depending', 'on', 'the', 'parameter... | [-0.1358570890852648, 0.1425779943945829, -0.07207327561330919, 0.05290875896287051, -0.06748525534408366, -0.18484320267311577, 0.08156075963334551, 0.33131806913184597, -0.23401915401364992, -0.28707254480896066, 0.06723590818396544, -0.23480730378114192, -0.21254315284912664, 0.0884617853331045, 0.003364899611661156... |
709.4206 | In silico network topology-based prediction of gene essentiality | The identification of genes essential for survival is important for the
understanding of the minimal requirements for cellular life and for drug
design. As experimental studies with the purpose of building a catalog of
essential genes for a given organism are time-consuming and laborious, a
computational approach whi... | q-bio.GN physics.bio-ph | the identification of genes essential for survival is important for the understanding of the minimal requirements for cellular life and for drug design as experimental studies with the purpose of building a catalog of essential genes for a given organism are timeconsuming and laborious a computational approach which co... | [['the', 'identification', 'of', 'genes', 'essential', 'for', 'survival', 'is', 'important', 'for', 'the', 'understanding', 'of', 'the', 'minimal', 'requirements', 'for', 'cellular', 'life', 'and', 'for', 'drug', 'design', 'as', 'experimental', 'studies', 'with', 'the', 'purpose', 'of', 'building', 'a', 'catalog', 'of'... | [-0.08782739662639996, 0.03767153967351199, -0.01238058193961537, 0.08633275431540999, -0.09457439785066216, -0.14831330231515402, 0.10928788977764786, 0.35965766130951554, -0.22140872343020004, -0.2779462203074665, 0.032267716140822474, -0.22244732689988964, -0.2607088456793195, 0.18429080305836115, -0.092415587362748... |
709.4207 | Deep study of the fast bipolar outflows in pre-PNe from CO mm-wave line
emission | High spatial resolution images of PNe have shown their extremely complex
morphology. However, the circumstellar envelopes of their progenitors, the AGB
stars, are strikingly spherical. In order to understand the carving processes
leading to axisymmetric nebulae, we are carrying out a study of a large sample
of pre-PN... | astro-ph | high spatial resolution images of pne have shown their extremely complex morphology however the circumstellar envelopes of their progenitors the agb stars are strikingly spherical in order to understand the carving processes leading to axisymmetric nebulae we are carrying out a study of a large sample of prepne our emi... | [['high', 'spatial', 'resolution', 'images', 'of', 'pne', 'have', 'shown', 'their', 'extremely', 'complex', 'morphology', 'however', 'the', 'circumstellar', 'envelopes', 'of', 'their', 'progenitors', 'the', 'agb', 'stars', 'are', 'strikingly', 'spherical', 'in', 'order', 'to', 'understand', 'the', 'carving', 'processes... | [-0.03958670635545097, 0.05560050224549145, -0.08638109751085847, 0.08291451767054868, -0.10831969724325784, -0.042763875034669864, 0.0061607626266777515, 0.4523836386646947, -0.19419208546329675, -0.3133224519611946, 0.055858144898906927, -0.23237490316788698, -0.0410807182097101, 0.17238136163936799, -0.0277834895341... |
709.4208 | Analysis of Flash ADC Data With VERITAS | VERITAS employs a 12m segmented mirror and pixellated photomultiplier tube
camera to detect the brief pulse of Cherenkov radiation produced by the
extensive air shower initiated by a cosmic high-energy gamma ray. The VERITAS
data acquisition system consists of a 500 Mega-Sample-Per-Second custom-built
flash ADC syste... | astro-ph | veritas employs a 12m segmented mirror and pixellated photomultiplier tube camera to detect the brief pulse of cherenkov radiation produced by the extensive air shower initiated by a cosmic highenergy gamma ray the veritas data acquisition system consists of a 500 megasamplepersecond custombuilt flash adc system which ... | [['veritas', 'employs', 'a', '12m', 'segmented', 'mirror', 'and', 'pixellated', 'photomultiplier', 'tube', 'camera', 'to', 'detect', 'the', 'brief', 'pulse', 'of', 'cherenkov', 'radiation', 'produced', 'by', 'the', 'extensive', 'air', 'shower', 'initiated', 'by', 'a', 'cosmic', 'highenergy', 'gamma', 'ray', 'the', 'ver... | [-0.08847631019892926, 0.15049635397176978, -0.05464121550264791, 0.07114582144862563, -0.016561555555487825, -0.1257369834560583, -0.02246767657357495, 0.4287473390946483, -0.19040138247173008, -0.38982656792305953, 0.11322844433513038, -0.34378330518417743, -0.0018612171875358355, 0.23503153130877763, -0.091183984459... |
709.4209 | Information capacity of genetic regulatory elements | Changes in a cell's external or internal conditions are usually reflected in
the concentrations of the relevant transcription factors. These proteins in
turn modulate the expression levels of the genes under their control and
sometimes need to perform non-trivial computations that integrate several
inputs and affect ... | q-bio.MN | changes in a cells external or internal conditions are usually reflected in the concentrations of the relevant transcription factors these proteins in turn modulate the expression levels of the genes under their control and sometimes need to perform nontrivial computations that integrate several inputs and affect multi... | [['changes', 'in', 'a', 'cells', 'external', 'or', 'internal', 'conditions', 'are', 'usually', 'reflected', 'in', 'the', 'concentrations', 'of', 'the', 'relevant', 'transcription', 'factors', 'these', 'proteins', 'in', 'turn', 'modulate', 'the', 'expression', 'levels', 'of', 'the', 'genes', 'under', 'their', 'control',... | [-0.16784163641863348, 0.1476143408663845, -0.012296434234759193, 0.08940774939477192, -0.04493841956558129, -0.16174482574195034, 0.12739113026135743, 0.3710197689000266, -0.27460676360521125, -0.2989300517251064, 0.08236956364329492, -0.23945834011016584, -0.19150114347272626, 0.1601597265557506, -0.09743551416818962... |
709.421 | Influence of Zeeman splitting and thermally excited polaron states on
magneto-electrical and magneto-thermal properties of magnetoresistive
polycrystalline manganite La_{0.8}Sr_{0.2}MnO_3 | Some possible connection between spin and charge degrees of freedom in
magneto-resistive manganites is investigated through a thorough experimental
study of the magnetic (AC susceptibility and DC magnetization) and transport
(resistivity and thermal conductivity) properties. Measurements are reported in
the case of w... | cond-mat.mtrl-sci | some possible connection between spin and charge degrees of freedom in magnetoresistive manganites is investigated through a thorough experimental study of the magnetic ac susceptibility and dc magnetization and transport resistivity and thermal conductivity properties measurements are reported in the case of well char... | [['some', 'possible', 'connection', 'between', 'spin', 'and', 'charge', 'degrees', 'of', 'freedom', 'in', 'magnetoresistive', 'manganites', 'is', 'investigated', 'through', 'a', 'thorough', 'experimental', 'study', 'of', 'the', 'magnetic', 'ac', 'susceptibility', 'and', 'dc', 'magnetization', 'and', 'transport', 'resis... | [-0.15250564054585994, 0.21365136922177044, -0.034593325532558894, 0.02247003825290853, -0.03905480496404279, -0.12724778535258438, 0.09008191651405974, 0.38995290526913273, -0.23670693391727077, -0.3011193545910323, 0.02544881958617932, -0.28774351458996533, -0.08780408769897703, 0.21064959273984035, 0.072425408763390... |
709.4211 | Chandra ACIS Survey of M33 (ChASeM33): A First Look | We present an overview of the Chandra ACIS Survey of M33 (ChASeM33): A Deep
Survey of the Nearest Face-on Spiral Galaxy. The 1.4 Ms survey covers the
galaxy out to $R \approx 18\arcmin (\approx 4$ kpc). These data provide the
most intensive, high spatial resolution assessment of the X-ray source
populations available... | astro-ph | we present an overview of the chandra acis survey of m33 chasem33 a deep survey of the nearest faceon spiral galaxy the 14 ms survey covers the galaxy out to r approx 18arcmin approx 4 kpc these data provide the most intensive high spatial resolution assessment of the xray source populations available for the confused ... | [['we', 'present', 'an', 'overview', 'of', 'the', 'chandra', 'acis', 'survey', 'of', 'm33', 'chasem33', 'a', 'deep', 'survey', 'of', 'the', 'nearest', 'faceon', 'spiral', 'galaxy', 'the', '14', 'ms', 'survey', 'covers', 'the', 'galaxy', 'out', 'to', 'r', 'approx', '18arcmin', 'approx', '4', 'kpc', 'these', 'data', 'pro... | [-0.032752723895988656, 0.04338502247803377, -0.03202891020712949, 0.14151140973274412, -0.0931665620108421, -0.029912217322179652, 0.08251167948295428, 0.45033580715782706, -0.16022218062357213, -0.3986749199079716, 0.06711632702737959, -0.38255598503861604, 0.03724750930601071, 0.20781820468919895, 0.0050408622867787... |
709.4212 | Exact diagonalization analysis of the Anderson-Hubbard model and
comparison to real-space self-consistent Hartree-Fock solutions | We have obtained the exact ground state wave functions of the
Anderson-Hubbard model for different electron fillings on a 4x4 lattice with
periodic boundary conditions - for 1/2 filling such ground states have roughly
166 million states. When compared to the uncorrelated ground states (Hubbard
interaction set to zero... | cond-mat.str-el cond-mat.dis-nn | we have obtained the exact ground state wave functions of the andersonhubbard model for different electron fillings on a 4x4 lattice with periodic boundary conditions for 12 filling such ground states have roughly 166 million states when compared to the uncorrelated ground states hubbard interaction set to zero we have... | [['we', 'have', 'obtained', 'the', 'exact', 'ground', 'state', 'wave', 'functions', 'of', 'the', 'andersonhubbard', 'model', 'for', 'different', 'electron', 'fillings', 'on', 'a', '4x4', 'lattice', 'with', 'periodic', 'boundary', 'conditions', 'for', '12', 'filling', 'such', 'ground', 'states', 'have', 'roughly', '166'... | [-0.14150372831436403, 0.16231576298502864, -0.05242218142783228, 0.1202222380284084, 0.04527330394820684, -0.137231752704693, 0.04366259200899542, 0.3937638791917014, -0.17698623274323821, -0.2952441727185119, 0.03730509486678226, -0.31109588891335754, -0.09371186026548763, 0.10367808519543087, 0.10675388743529898, 0.... |
709.4213 | Hamiltonian Lattice QCD near the Light Cone | We give a status report of our work on light cone Hamiltonian lattice QCD. We
have derived an effective Hamiltonian $H_{eff}$ which is only quadratic in the
momenta and therefore can be simulated by standard methods. For this
Hamiltonian we determine variationally an approximate ground state wave
functional in the li... | hep-lat | we give a status report of our work on light cone hamiltonian lattice qcd we have derived an effective hamiltonian h_eff which is only quadratic in the momenta and therefore can be simulated by standard methods for this hamiltonian we determine variationally an approximate ground state wave functional in the light cone... | [['we', 'give', 'a', 'status', 'report', 'of', 'our', 'work', 'on', 'light', 'cone', 'hamiltonian', 'lattice', 'qcd', 'we', 'have', 'derived', 'an', 'effective', 'hamiltonian', 'h_eff', 'which', 'is', 'only', 'quadratic', 'in', 'the', 'momenta', 'and', 'therefore', 'can', 'be', 'simulated', 'by', 'standard', 'methods',... | [-0.1372193311218102, 0.14703062282631368, -0.1236252241926092, 0.061260530654833, -0.06344388100705198, -0.07941023600375596, 0.05668332480456469, 0.3979652256195275, -0.24417101397653515, -0.26253113586385296, 0.07685779904472237, -0.2587904014255641, -0.1439080929453924, 0.1688849483177347, -0.0020739823439211214, 0... |
709.4214 | Destruction of first-order phase transition in a random-field Ising
model | The phase transitions that occur in an infinite-range-interaction Ising
ferromagnet in the presence of a double-Gaussian random magnetic field are
analyzed. Such random fields are defined as a superposition of two Gaussian
distributions, presenting the same width $\sigma$. Is is argued that this
distribution is more ... | cond-mat.dis-nn cond-mat.stat-mech | the phase transitions that occur in an infiniterangeinteraction ising ferromagnet in the presence of a doublegaussian random magnetic field are analyzed such random fields are defined as a superposition of two gaussian distributions presenting the same width sigma is is argued that this distribution is more appropriate... | [['the', 'phase', 'transitions', 'that', 'occur', 'in', 'an', 'infiniterangeinteraction', 'ising', 'ferromagnet', 'in', 'the', 'presence', 'of', 'a', 'doublegaussian', 'random', 'magnetic', 'field', 'are', 'analyzed', 'such', 'random', 'fields', 'are', 'defined', 'as', 'a', 'superposition', 'of', 'two', 'gaussian', 'di... | [-0.14889896017244472, 0.2391146678273799, -0.09465335173760804, 0.09987129060604241, -0.025888051723463916, -0.14590523516284828, 0.01978097260898893, 0.3895215853205267, -0.2369218437299835, -0.23121086766345883, 0.059671281410802926, -0.27308748235469155, -0.13174366106648208, 0.1451738283987034, 0.00379700224763133... |
709.4215 | Multiplicity one Theorems | In the local, characteristic 0, non archimedean case, we consider
distributions on GL(n+1) which are invariant under the adjoint action of GL(n).
We prove that such distributions are invariant by transposition. This implies
that an admissible irreducible representation of GL(n+1), when restricted to
GL(n) decomposes ... | math.RT | in the local characteristic 0 non archimedean case we consider distributions on gln1 which are invariant under the adjoint action of gln we prove that such distributions are invariant by transposition this implies that an admissible irreducible representation of gln1 when restricted to gln decomposes with multiplicity ... | [['in', 'the', 'local', 'characteristic', '0', 'non', 'archimedean', 'case', 'we', 'consider', 'distributions', 'on', 'gln1', 'which', 'are', 'invariant', 'under', 'the', 'adjoint', 'action', 'of', 'gln', 'we', 'prove', 'that', 'such', 'distributions', 'are', 'invariant', 'by', 'transposition', 'this', 'implies', 'that... | [-0.17173884533705158, 0.15709359397148723, -0.14162762969601572, 0.07363594675297734, -0.05314908532850575, -0.1368713396552362, -0.08775254877349525, 0.36963323457983505, -0.2890062139679988, -0.14124794082160583, 0.08041726282119685, -0.22567289152689146, -0.10770613591088668, 0.17268729416996634, -0.086307066909380... |
709.4216 | Critical structure of the QCD medium | Fluctuations in the vicinity of a phase transition are important but
neglected in mean-field theory. In order to assess the influence of such
fluctuations on the critical endpoint and the size of the critical region in
the QCD phase diagram, a mean-field calculation of a two-flavor quark-meson
model is compared with ... | hep-ph | fluctuations in the vicinity of a phase transition are important but neglected in meanfield theory in order to assess the influence of such fluctuations on the critical endpoint and the size of the critical region in the qcd phase diagram a meanfield calculation of a twoflavor quarkmeson model is compared with a renorm... | [['fluctuations', 'in', 'the', 'vicinity', 'of', 'a', 'phase', 'transition', 'are', 'important', 'but', 'neglected', 'in', 'meanfield', 'theory', 'in', 'order', 'to', 'assess', 'the', 'influence', 'of', 'such', 'fluctuations', 'on', 'the', 'critical', 'endpoint', 'and', 'the', 'size', 'of', 'the', 'critical', 'region',... | [-0.15210839520390754, 0.198109077475965, -0.11633452119548683, 0.06413078273788257, -0.01598200039614154, -0.06509618197527269, 0.10773369646125028, 0.3249810776470796, -0.20517784724740878, -0.28378194134844387, 0.07882109690437336, -0.2709741642739138, -0.137058234255275, 0.07151154317164227, 0.003886661194416735, 0... |
709.4217 | Weak measurement and control of entanglement generation | In this paper we show how weak joint measurement and local feedback can be
used to control entanglement generation between two qubits. To do this, we make
use of a decoherence free subspace (DFS). Weak measurement and feedback can be
used to drive the system into this subspace rapidly. Once within the subspace,
feedb... | quant-ph | in this paper we show how weak joint measurement and local feedback can be used to control entanglement generation between two qubits to do this we make use of a decoherence free subspace dfs weak measurement and feedback can be used to drive the system into this subspace rapidly once within the subspace feedback can g... | [['in', 'this', 'paper', 'we', 'show', 'how', 'weak', 'joint', 'measurement', 'and', 'local', 'feedback', 'can', 'be', 'used', 'to', 'control', 'entanglement', 'generation', 'between', 'two', 'qubits', 'to', 'do', 'this', 'we', 'make', 'use', 'of', 'a', 'decoherence', 'free', 'subspace', 'dfs', 'weak', 'measurement', '... | [-0.12435057280976096, 0.20035972815282918, -0.06333026029514494, 0.07000030961353332, -0.026783363778650024, -0.17333137875790766, 0.05993456402247381, 0.40076624307735464, -0.33829461378447806, -0.2666787757239316, 0.09311079161736056, -0.2371143409838601, -0.09300189565602736, 0.19131343118288774, -0.064288058102613... |
709.4218 | A Monolithic Pixel Sensor in 0.15 micron Fully Depleted SOI Technology | This letter presents the design of a monolithic pixel sensor with 10x10
micron^2 pixels in OKI 0.15 micron fully depleted SOI technology and first
results of its characterisation. The response of the chip to charged particles
has been studied on the 1.35 GeV electron beam at the LBNL ALS.
| physics.ins-det | this letter presents the design of a monolithic pixel sensor with 10x10 micron2 pixels in oki 015 micron fully depleted soi technology and first results of its characterisation the response of the chip to charged particles has been studied on the 135 gev electron beam at the lbnl als | [['this', 'letter', 'presents', 'the', 'design', 'of', 'a', 'monolithic', 'pixel', 'sensor', 'with', '10x10', 'micron2', 'pixels', 'in', 'oki', '015', 'micron', 'fully', 'depleted', 'soi', 'technology', 'and', 'first', 'results', 'of', 'its', 'characterisation', 'the', 'response', 'of', 'the', 'chip', 'to', 'charged', ... | [-0.0660103833711497, 0.13711349712209586, -0.0037649687360592037, -0.10731808915829325, 0.049631577536311686, -0.1659276621150119, -0.013953849065060519, 0.44594041166865095, -0.1460824049629119, -0.3699848715748106, 0.0422805579526502, -0.33074392037162065, -0.001967220890278719, 0.1363597890286117, -0.09943900006462... |
709.4219 | Is the sky falling? Searching for stellar streams in the local Milky Way
disc in the CORAVEL and RAVE surveys | We have searched for in-falling stellar streams on to the local Milky Way
disc in the CORAVEL and RAVE surveys. The CORAVEL survey consists of local
dwarf stars (Nordstrom et al. Geneva-Copenhagen survey) and local Famaey et al.
giant stars. We select RAVE stars with radial velocities that are sensitive to
the Galact... | astro-ph | we have searched for infalling stellar streams on to the local milky way disc in the coravel and rave surveys the coravel survey consists of local dwarf stars nordstrom et al genevacopenhagen survey and local famaey et al giant stars we select rave stars with radial velocities that are sensitive to the galactic vertica... | [['we', 'have', 'searched', 'for', 'infalling', 'stellar', 'streams', 'on', 'to', 'the', 'local', 'milky', 'way', 'disc', 'in', 'the', 'coravel', 'and', 'rave', 'surveys', 'the', 'coravel', 'survey', 'consists', 'of', 'local', 'dwarf', 'stars', 'nordstrom', 'et', 'al', 'genevacopenhagen', 'survey', 'and', 'local', 'fam... | [-0.08295829249545932, 0.11039151752020343, -0.06994789780672024, 0.058459572349990704, -0.12173758471459624, 0.03841083030042759, 0.07235330518777087, 0.36419763928752835, -0.16566159414103793, -0.3896944384958784, -0.013885685476431054, -0.31670447501306564, 0.004567472852955935, 0.21534100295383862, -0.0594873333618... |
709.422 | Non-thermal emission processes in massive binaries | In this paper, I present a general discussion of several astrophysical
processes likely to play a role in the production of non-thermal emission in
massive stars, with emphasis on massive binaries. Even though the discussion
will start in the radio domain where the non-thermal emission was first
detected, the census ... | astro-ph | in this paper i present a general discussion of several astrophysical processes likely to play a role in the production of nonthermal emission in massive stars with emphasis on massive binaries even though the discussion will start in the radio domain where the nonthermal emission was first detected the census of physi... | [['in', 'this', 'paper', 'i', 'present', 'a', 'general', 'discussion', 'of', 'several', 'astrophysical', 'processes', 'likely', 'to', 'play', 'a', 'role', 'in', 'the', 'production', 'of', 'nonthermal', 'emission', 'in', 'massive', 'stars', 'with', 'emphasis', 'on', 'massive', 'binaries', 'even', 'though', 'the', 'discu... | [-0.07319484631703961, 0.16257191164666837, -0.0465015804548876, 0.14919319073082196, -0.12138452575704374, -0.06760595801260767, 0.03260009698228005, 0.40411898102013205, -0.18654359232072523, -0.3065420697708059, 0.0661893322628094, -0.28843769880968634, -0.05750920449879123, 0.2326307876095381, -0.023288730757285353... |
709.4221 | NNLO QCD corrections to event shape variables in electron positron
annihilation | Precision studies of QCD at electron-positron colliders are based on
measurements of event shapes and jet rates. To match the high experimental
accuracy, theoretical predictions to next-to-next-to-leading order (NNLO) in
QCD are needed for a reliable interpretation of the data. We report the first
calculation of NNLO... | hep-ph | precision studies of qcd at electronpositron colliders are based on measurements of event shapes and jet rates to match the high experimental accuracy theoretical predictions to nexttonexttoleading order nnlo in qcd are needed for a reliable interpretation of the data we report the first calculation of nnlo corrections... | [['precision', 'studies', 'of', 'qcd', 'at', 'electronpositron', 'colliders', 'are', 'based', 'on', 'measurements', 'of', 'event', 'shapes', 'and', 'jet', 'rates', 'to', 'match', 'the', 'high', 'experimental', 'accuracy', 'theoretical', 'predictions', 'to', 'nexttonexttoleading', 'order', 'nnlo', 'in', 'qcd', 'are', 'n... | [-0.06821833107025042, 0.07498356032750157, -0.1184462735841631, 0.14794695785757703, -0.08617976217790217, -0.03362432816142186, 0.03428405749260402, 0.41627245652871053, -0.09253976788738223, -0.2993423632483502, 0.047951471516633495, -0.39441478838686084, 0.05391264083169279, 0.1665701265217828, 0.0478011901169771, ... |
709.4222 | Archimedes' balance and Bianchi's Backlund transformation for quadrics | We establish a link between Archimedes' method of integration for calculating
areas, volumes and centers of mass of segments of parabolas and quadrics of
revolution by factorization via the moments of a balance and an integration
technique for a particular integrable system, namely Bianchi's B\"{a}cklund
transformati... | math.DG | we establish a link between archimedes method of integration for calculating areas volumes and centers of mass of segments of parabolas and quadrics of revolution by factorization via the moments of a balance and an integration technique for a particular integrable system namely bianchis backlund transformation for qua... | [['we', 'establish', 'a', 'link', 'between', 'archimedes', 'method', 'of', 'integration', 'for', 'calculating', 'areas', 'volumes', 'and', 'centers', 'of', 'mass', 'of', 'segments', 'of', 'parabolas', 'and', 'quadrics', 'of', 'revolution', 'by', 'factorization', 'via', 'the', 'moments', 'of', 'a', 'balance', 'and', 'an... | [-0.16691632120152158, -0.0016738474244751462, -0.08060455970310916, 0.0766635152103845, -0.011206708188789586, -0.10026010518777184, 0.053129449714712486, 0.3603649950867596, -0.2847743745272358, -0.25462795386556536, 0.11308199042105116, -0.2969585322619726, -0.1657338683338215, 0.2339693793813543, -0.047271642892155... |
709.4223 | Measurement of the Open Charm Cross-Section in $\sqrt{s_{NN}}$ = 200 GeV
Cu+Cu Collisions at STAR | We present the mid-rapidity $(D^{0} + \bar{D^{0}})/2$ yield measured in
$\sqrt{s_{NN}}$ = 200 GeV Cu+Cu collisions at RHIC via direct reconstruction
through the $K\pi$ decay channel. A charm cross-section is reported and
compared to theoretical predictions and to previous RHIC experimental results.
| nucl-ex | we present the midrapidity d0 bard02 yield measured in sqrts_nn 200 gev cucu collisions at rhic via direct reconstruction through the kpi decay channel a charm crosssection is reported and compared to theoretical predictions and to previous rhic experimental results | [['we', 'present', 'the', 'midrapidity', 'd0', 'bard02', 'yield', 'measured', 'in', 'sqrts_nn', '200', 'gev', 'cucu', 'collisions', 'at', 'rhic', 'via', 'direct', 'reconstruction', 'through', 'the', 'kpi', 'decay', 'channel', 'a', 'charm', 'crosssection', 'is', 'reported', 'and', 'compared', 'to', 'theoretical', 'predi... | [-0.024840195508052904, 0.22852363396818057, -0.23376936075062707, 0.10821958472773147, 0.018703102892360244, -0.14290645526339993, -0.06930302769447175, 0.3582344504121022, -0.19994103660186133, -0.25455217989973533, -0.15065949264233217, -0.46297605870625913, 0.20351994463887352, 0.2071525322703215, 0.125409377332872... |
709.4224 | Methods for Pseudoscalar Flavour-Singlet Mesons with Staggered Fermions | We present the first 2+1 flavour lattice QCD calculations of pseudoscalar
flavour-singlet propagators using improved staggered fermions. We explore the
relevant techniques and discuss prospects for the larger scale studies now in
progress. The disconnected correlator is shown to have a highly non-Gaussian
distributio... | hep-lat | we present the first 21 flavour lattice qcd calculations of pseudoscalar flavoursinglet propagators using improved staggered fermions we explore the relevant techniques and discuss prospects for the larger scale studies now in progress the disconnected correlator is shown to have a highly nongaussian distribution and r... | [['we', 'present', 'the', 'first', '21', 'flavour', 'lattice', 'qcd', 'calculations', 'of', 'pseudoscalar', 'flavoursinglet', 'propagators', 'using', 'improved', 'staggered', 'fermions', 'we', 'explore', 'the', 'relevant', 'techniques', 'and', 'discuss', 'prospects', 'for', 'the', 'larger', 'scale', 'studies', 'now', '... | [-0.11877927570738113, 0.22411977844491887, -0.09360837177015267, 0.13345743519871925, -0.058554664809400074, -0.10775749311477949, 0.07432910453868456, 0.40500585494849545, -0.1096226326816787, -0.22825416893913195, 0.11866738395362447, -0.2714528125316764, -0.08752487663430376, 0.14635824990154317, 0.0499933932442218... |
709.4225 | The status of Quantum Geometry in the dynamical sector of Loop Quantum
Cosmology | This letter is motivated by the recent papers by Dittrich and Thiemann and,
respectively, by Rovelli discussing the status of Quantum Geometry in the
dynamical sector of Loop Quantum Gravity. Since the papers consider model
examples, we also study the issue in the case of an example, namely on the Loop
Quantum Cosmol... | gr-qc hep-th | this letter is motivated by the recent papers by dittrich and thiemann and respectively by rovelli discussing the status of quantum geometry in the dynamical sector of loop quantum gravity since the papers consider model examples we also study the issue in the case of an example namely on the loop quantum cosmology mod... | [['this', 'letter', 'is', 'motivated', 'by', 'the', 'recent', 'papers', 'by', 'dittrich', 'and', 'thiemann', 'and', 'respectively', 'by', 'rovelli', 'discussing', 'the', 'status', 'of', 'quantum', 'geometry', 'in', 'the', 'dynamical', 'sector', 'of', 'loop', 'quantum', 'gravity', 'since', 'the', 'papers', 'consider', '... | [-0.12023537548308351, 0.1158588430371632, -0.0864476507068076, 0.08570010013120101, -0.04397976032532422, -0.10241694779411387, -0.0018211300835112292, 0.2845560444469473, -0.25334435157205876, -0.2638389857865013, 0.11103223098248276, -0.25939509319553594, -0.17312950954104947, 0.20097087059722207, -0.088836158337318... |
709.4226 | Tent Spaces Associated with Semigroups of Operators | We study tent spaces on general measure spaces $(\Omega, \mu)$. We assume
that there exists a semigroup of positive operators on $L^p(\Omega, \mu)$
satisfying a monotone property but do not assume any geometric/metric structure
on $\Omega$. The semigroup plays the same role as integrals on cones and cubes
in Euclidea... | math.FA math.CA | we study tent spaces on general measure spaces omega mu we assume that there exists a semigroup of positive operators on lpomega mu satisfying a monotone property but do not assume any geometricmetric structure on omega the semigroup plays the same role as integrals on cones and cubes in euclidean spaces we then study ... | [['we', 'study', 'tent', 'spaces', 'on', 'general', 'measure', 'spaces', 'omega', 'mu', 'we', 'assume', 'that', 'there', 'exists', 'a', 'semigroup', 'of', 'positive', 'operators', 'on', 'lpomega', 'mu', 'satisfying', 'a', 'monotone', 'property', 'but', 'do', 'not', 'assume', 'any', 'geometricmetric', 'structure', 'on',... | [-0.1254455106884339, 0.08950124073323279, -0.09304172159907849, 0.20977629409416726, -0.0984397472084598, -0.12083642906754424, 0.009978059986851326, 0.3943453438776104, -0.2968371360121589, -0.10567603298511945, 0.14791082283727042, -0.29635102396928953, -0.15477948765221394, 0.21361539810773378, -0.1447865121262638,... |
709.4227 | Scalar Particle Contribution to Higgs Production via Gluon Fusion at NLO | We consider the gluon fusion production cross section of a scalar Higgs boson
in models where fermion and scalar massive colored particles are present. We
report analytic expressions for the matrix elements of $gg\to Hg$, $q\bar{q}\to
Hg$, and $qg\to Hq$ processes completing the calculation of the NLO QCD
corrections... | hep-ph | we consider the gluon fusion production cross section of a scalar higgs boson in models where fermion and scalar massive colored particles are present we report analytic expressions for the matrix elements of ggto hg qbarqto hg and qgto hq processes completing the calculation of the nlo qcd corrections in these extende... | [['we', 'consider', 'the', 'gluon', 'fusion', 'production', 'cross', 'section', 'of', 'a', 'scalar', 'higgs', 'boson', 'in', 'models', 'where', 'fermion', 'and', 'scalar', 'massive', 'colored', 'particles', 'are', 'present', 'we', 'report', 'analytic', 'expressions', 'for', 'the', 'matrix', 'elements', 'of', 'ggto', 'h... | [-0.07598804294910474, 0.2012044088312842, -0.04273237541703315, 0.14574558721506037, -0.05773237584849242, -0.14773725235336943, -0.012401455774469751, 0.33179835883643605, -0.15322600445581663, -0.20055954526017966, -0.013553646607886487, -0.29520706338245933, -0.0562892422754446, 0.11107773708524825, 0.0426643338654... |
709.4228 | Spectral properties in the charge density wave phase of the half-filled
Falicov-Kimball Model | We study the spectral properties of charge density wave (CDW) phase of the
half-filled spinless Falicov-Kimball model within the framework of the
Dynamical Mean Field Theory. We present detailed results for the spectral
function in the CDW phase as function of temperature and $U$. We show how the
proximity of the non... | cond-mat.str-el | we study the spectral properties of charge density wave cdw phase of the halffilled spinless falicovkimball model within the framework of the dynamical mean field theory we present detailed results for the spectral function in the cdw phase as function of temperature and u we show how the proximity of the nonfermi liqu... | [['we', 'study', 'the', 'spectral', 'properties', 'of', 'charge', 'density', 'wave', 'cdw', 'phase', 'of', 'the', 'halffilled', 'spinless', 'falicovkimball', 'model', 'within', 'the', 'framework', 'of', 'the', 'dynamical', 'mean', 'field', 'theory', 'we', 'present', 'detailed', 'results', 'for', 'the', 'spectral', 'fun... | [-0.16811805560719223, 0.1788871891773306, -0.11637290382059291, 0.06311399586731568, -0.00564214245416224, -0.04740221475833096, 0.12500588889117353, 0.35651952493935823, -0.2570252872724086, -0.23980691203847526, 0.025662243851693346, -0.3185170940030366, -0.19213982664979995, 0.06910504014929757, 0.03442323319119168... |
709.4229 | An Extrapolation of Operator Valued Dyadic Paraproducts | We consider the dyadic paraproducts $\pi_\f$ on $\T$ associated with an
$\M$-valued function $\f.$ Here $\T$ is the unit circle and $\M$ is a tracial
von Neumann algebra. We prove that their boundedness on $L^p(\T,L^p(\M))$ for
some $1<p<\infty $ implies their boundedness on $L^p(\T,L^p(\M))$ for all
$1<p<\infty$ pro... | math.FA math.CA | we consider the dyadic paraproducts pi_f on t associated with an mvalued function f here t is the unit circle and m is a tracial von neumann algebra we prove that their boundedness on lptlpm for some 1pinfty implies their boundedness on lptlpm for all 1pinfty provided f is in an operatorvalued bmo space we also conside... | [['we', 'consider', 'the', 'dyadic', 'paraproducts', 'pi_f', 'on', 't', 'associated', 'with', 'an', 'mvalued', 'function', 'f', 'here', 't', 'is', 'the', 'unit', 'circle', 'and', 'm', 'is', 'a', 'tracial', 'von', 'neumann', 'algebra', 'we', 'prove', 'that', 'their', 'boundedness', 'on', 'lptlpm', 'for', 'some', '1pinft... | [-0.15653021913021803, 0.11169179899126688, -0.049918969682253456, 0.10721999703844845, -0.1163508420029436, -0.09403043959344573, -0.01708856491399381, 0.3904948685393559, -0.33726431045900374, -0.07565998233964338, 0.16671666598652818, -0.314970177694169, -0.08349541878765997, 0.23068130563136519, -0.1858376506921451... |
709.423 | Lower bounds on the blow-up rate of the axisymmetric Navier-Stokes
equations II | Consider axisymmetric strong solutions of the incompressible Navier-Stokes
equations in $\R^3$ with non-trivial swirl. Let $z$ denote the axis of symmetry
and $r$ measure the distance to the z-axis. Suppose the solution satisfies
either $|v (x,t)| \le C_*{|t|^{-1/2}} $ or, for some $\e > 0$, $|v (x,t)| \le
C_* r^{-1+... | math.AP | consider axisymmetric strong solutions of the incompressible navierstokes equations in r3 with nontrivial swirl let z denote the axis of symmetry and r measure the distance to the zaxis suppose the solution satisfies either v xt le c_t12 or for some e 0 v xt le c_ r1epsilon tepsilon 2 for t_0le t 0 and 0c_infty allowed... | [['consider', 'axisymmetric', 'strong', 'solutions', 'of', 'the', 'incompressible', 'navierstokes', 'equations', 'in', 'r3', 'with', 'nontrivial', 'swirl', 'let', 'z', 'denote', 'the', 'axis', 'of', 'symmetry', 'and', 'r', 'measure', 'the', 'distance', 'to', 'the', 'zaxis', 'suppose', 'the', 'solution', 'satisfies', 'e... | [-0.2521741110231784, 0.13888994817424452, -0.02270952289020925, -0.026762549460258786, -0.054750319781967184, -0.2665041849955521, -0.034002070371626, 0.3007404939518451, -0.34609683524027013, -0.1703138383190063, 0.07305299659845221, -0.3646018585246621, 0.029618203763454927, 0.10410984133892326, -0.00356058504037333... |
709.4231 | On the anatomy of multi-spin magnon and single spike string solutions | We study rigid string solutions rotating in $AdS_5\times S^5$ background. For
particular values of the parameters of the solutions we find multispin
solutions corresponding to giant magnons and single spike strings. We present
an analysis of the dispersion relations in the case of three spin solutions
distributed onl... | hep-th | we study rigid string solutions rotating in ads_5times s5 background for particular values of the parameters of the solutions we find multispin solutions corresponding to giant magnons and single spike strings we present an analysis of the dispersion relations in the case of three spin solutions distributed only in s5 ... | [['we', 'study', 'rigid', 'string', 'solutions', 'rotating', 'in', 'ads_5times', 's5', 'background', 'for', 'particular', 'values', 'of', 'the', 'parameters', 'of', 'the', 'solutions', 'we', 'find', 'multispin', 'solutions', 'corresponding', 'to', 'giant', 'magnons', 'and', 'single', 'spike', 'strings', 'we', 'present'... | [-0.20258237468660809, 0.14334323697275977, -0.0036513963248580696, 0.11118836255045608, -0.04817490816058125, -0.10325793921947479, -0.013338021664822008, 0.36326774444896726, -0.18099226276390254, -0.2263472194550559, 0.12239038639672799, -0.3361834611161612, -0.09910952458158136, 0.16626801975653507, -0.012658466189... |
709.4232 | Q-manifolds and Mackenzie theory: an overview | This text is meant to be a brief overview of the topics announced in the
title and is based on my talk in Vienna (August/September 2007). It does not
contain new results (except probably for a remark concerning Q-manifold
homology, which I wish to elaborate elsewhere).
"Mackenzie theory" stands for the rich circle ... | math.DG math-ph math.MP math.SG | this text is meant to be a brief overview of the topics announced in the title and is based on my talk in vienna augustseptember 2007 it does not contain new results except probably for a remark concerning qmanifold homology which i wish to elaborate elsewhere mackenzie theory stands for the rich circle of notions that... | [['this', 'text', 'is', 'meant', 'to', 'be', 'a', 'brief', 'overview', 'of', 'the', 'topics', 'announced', 'in', 'the', 'title', 'and', 'is', 'based', 'on', 'my', 'talk', 'in', 'vienna', 'augustseptember', '2007', 'it', 'does', 'not', 'contain', 'new', 'results', 'except', 'probably', 'for', 'a', 'remark', 'concerning'... | [-0.1509798201430287, 0.090251091922196, -0.10296345807445186, 0.1412802039582685, -0.1925874428269831, -0.20062271612570495, 0.0018562119674390635, 0.374837507237051, -0.2909568474904911, -0.24906006258333455, 0.09071322420007877, -0.21060176724693863, -0.1928988064400147, 0.16953985218707524, -0.1624848974560312, -0.... |
709.4233 | VEGAS, the VERITAS Gamma-ray Analysis Suite | VERITAS, the Very Energetic Radiation Imaging Telescope Array System, is an
array of four 12 m diameter imaging atmospheric Cherenkov telescopes for
gamma-ray astronomy above 100 GeV currently in operation in Arizona. The
VERITAS Collaboration has developed VEGAS, the VERITAS Gamma-ray Analysis
Suite, a data-analysis... | astro-ph | veritas the very energetic radiation imaging telescope array system is an array of four 12 m diameter imaging atmospheric cherenkov telescopes for gammaray astronomy above 100 gev currently in operation in arizona the veritas collaboration has developed vegas the veritas gammaray analysis suite a dataanalysis software ... | [['veritas', 'the', 'very', 'energetic', 'radiation', 'imaging', 'telescope', 'array', 'system', 'is', 'an', 'array', 'of', 'four', '12', 'm', 'diameter', 'imaging', 'atmospheric', 'cherenkov', 'telescopes', 'for', 'gammaray', 'astronomy', 'above', '100', 'gev', 'currently', 'in', 'operation', 'in', 'arizona', 'the', '... | [-0.11124221380265761, 0.09754889909380618, -0.06115431156615878, 0.08053901734267355, -0.07206781651073879, -0.1648320182183281, -0.07067165040057297, 0.42453975894654444, -0.20150666863679192, -0.427075122510148, 0.15626519303064967, -0.27632904383750967, -0.07879986749716507, 0.284986765995665, 0.022258173807906782,... |
709.4234 | Cosmological bounds on oscillating dark energy models | We study some cosmological constraints on the two phenomenological models of
oscillating dark energy. In these scenarios, the equation of state of dark
energy varies periodically and may provide a way to unify the early
acceleration (inflation) and the late time acceleration of the universe. These
models give also an... | astro-ph | we study some cosmological constraints on the two phenomenological models of oscillating dark energy in these scenarios the equation of state of dark energy varies periodically and may provide a way to unify the early acceleration inflation and the late time acceleration of the universe these models give also an effect... | [['we', 'study', 'some', 'cosmological', 'constraints', 'on', 'the', 'two', 'phenomenological', 'models', 'of', 'oscillating', 'dark', 'energy', 'in', 'these', 'scenarios', 'the', 'equation', 'of', 'state', 'of', 'dark', 'energy', 'varies', 'periodically', 'and', 'may', 'provide', 'a', 'way', 'to', 'unify', 'the', 'ear... | [-0.1123828284596045, 0.08626837968558058, -0.08511691186193031, 0.12383491159704774, -0.16432139671110002, -0.08518812328711459, 0.02829313346367214, 0.3031146532577491, -0.27124978317015025, -0.3551258897773691, 0.07983196742434208, -0.29844945851598204, -0.011808429278202892, 0.23275686888811514, -0.0066862109606424... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.