id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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710.2653 | A Supersymmetric U(1)' Model with Multiple Dark Matters | We consider a scenario where a supersymmetric model has multiple dark matter
particles. Adding a U(1)' gauge symmetry is a well-motivated extension of the
Minimal Supersymmetric Standard Model (MSSM). It can cure the problems of the
MSSM such as the mu-problem or the proton decay problem with high-dimensional
lepton ... | hep-ph | we consider a scenario where a supersymmetric model has multiple dark matter particles adding a u1 gauge symmetry is a wellmotivated extension of the minimal supersymmetric standard model mssm it can cure the problems of the mssm such as the muproblem or the proton decay problem with highdimensional lepton number and b... | [['we', 'consider', 'a', 'scenario', 'where', 'a', 'supersymmetric', 'model', 'has', 'multiple', 'dark', 'matter', 'particles', 'adding', 'a', 'u1', 'gauge', 'symmetry', 'is', 'a', 'wellmotivated', 'extension', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'it', 'can', 'cure', 'the', 'problems'... | [-0.14355340833118296, 0.24255405926113086, -0.0693343753926456, 0.15336755903862306, -0.13371335485100966, -0.21780852891936187, 0.0035835159902275976, 0.26547168908394214, -0.21410500186988535, -0.34976126411655806, 0.06343249231303001, -0.25851647875088557, -0.05128811465932385, 0.08593782850143993, 0.01963934337254... |
710.2654 | Stellar explosions powered by the Blandford-Znajek mechanism | In this letter we briefly describe the first results of our numerical study
on the possibility of magnetic origin of relativistic jets of long duration
gamma ray bursters within the collapsar scenario. We track the collapse of
massive rotating stars onto a rotating central black hole using axisymmetric
general relati... | astro-ph | in this letter we briefly describe the first results of our numerical study on the possibility of magnetic origin of relativistic jets of long duration gamma ray bursters within the collapsar scenario we track the collapse of massive rotating stars onto a rotating central black hole using axisymmetric general relativis... | [['in', 'this', 'letter', 'we', 'briefly', 'describe', 'the', 'first', 'results', 'of', 'our', 'numerical', 'study', 'on', 'the', 'possibility', 'of', 'magnetic', 'origin', 'of', 'relativistic', 'jets', 'of', 'long', 'duration', 'gamma', 'ray', 'bursters', 'within', 'the', 'collapsar', 'scenario', 'we', 'track', 'the',... | [-0.11630562073374286, 0.14940606295779535, -0.04580847704282054, 0.12950027398057753, -0.08557811324319602, -0.08245565344489628, 0.010630726832690165, 0.35335253266311145, -0.20043771077961295, -0.2954437975547736, 0.052598091168771205, -0.27595960231250316, -0.018235263744769973, 0.23226167492515443, 0.0070452128958... |
710.2655 | Detailed Studies of Pixelated CZT Detectors Grown with the Modified
Horizontal Bridgman Method | The detector material Cadmium Zinc Telluride (CZT), known for its high
resolution over a broad energy range, is produced mainly by two methods: the
Modified High-Pressure Bridgman (MHB) and the High-Pressure Bridgman (HPB)
process. This study is based on MHB CZT substrates from the company Orbotech
Medical Solutions ... | astro-ph | the detector material cadmium zinc telluride czt known for its high resolution over a broad energy range is produced mainly by two methods the modified highpressure bridgman mhb and the highpressure bridgman hpb process this study is based on mhb czt substrates from the company orbotech medical solutions ltd with a det... | [['the', 'detector', 'material', 'cadmium', 'zinc', 'telluride', 'czt', 'known', 'for', 'its', 'high', 'resolution', 'over', 'a', 'broad', 'energy', 'range', 'is', 'produced', 'mainly', 'by', 'two', 'methods', 'the', 'modified', 'highpressure', 'bridgman', 'mhb', 'and', 'the', 'highpressure', 'bridgman', 'hpb', 'proces... | [-0.011099021159612608, 0.134929870572631, 0.027653221337607614, 0.011017959419007605, 0.01026980183777158, -0.15679393707153697, 0.0729377804858679, 0.43415386166285586, -0.18554736859406587, -0.41005569490155686, 0.06226213427467479, -0.37004266517167844, -0.0013498825840307055, 0.21625634272824282, -0.01996724294860... |
710.2656 | Pioneer Anomaly: Evaluating Newly Recovered Data | The Pioneer 10/11 spacecraft yielded the most precise navigation in deep
space to date. However, their radio-metric tracking data received from the
distances between 20--70 astronomical units from the Sun consistently indicated
the presence of a small, anomalous, Doppler frequency drift. The drift is a
blue frequency... | gr-qc | the pioneer 1011 spacecraft yielded the most precise navigation in deep space to date however their radiometric tracking data received from the distances between 2070 astronomical units from the sun consistently indicated the presence of a small anomalous doppler frequency drift the drift is a blue frequency shift that... | [['the', 'pioneer', '1011', 'spacecraft', 'yielded', 'the', 'most', 'precise', 'navigation', 'in', 'deep', 'space', 'to', 'date', 'however', 'their', 'radiometric', 'tracking', 'data', 'received', 'from', 'the', 'distances', 'between', '2070', 'astronomical', 'units', 'from', 'the', 'sun', 'consistently', 'indicated', ... | [-0.10655327408937161, 0.13401225901752775, -0.08513917726784197, 0.03684098441699783, -0.1398571404850984, -0.09184248408043048, 0.027645987089706864, 0.3681670622374714, -0.24944311249599405, -0.3836648647871231, 0.11792837242509313, -0.29784074419309936, -0.0979100050565898, 0.23321305019101046, -0.10401050914476875... |
710.2657 | Non-Newtonian viscosity in magnetized plasma | The particle and momentum balance equations can be solved on concentric
circular flux surfaces to determine the effective viscous drag present in a
magnetized tokamak plasma in the low aspect ratio limit. An analysis is
developed utilizing the first-order Fourier expansion of the poloidal variation
of quantities on t... | physics.plasm-ph | the particle and momentum balance equations can be solved on concentric circular flux surfaces to determine the effective viscous drag present in a magnetized tokamak plasma in the low aspect ratio limit an analysis is developed utilizing the firstorder fourier expansion of the poloidal variation of quantities on the f... | [['the', 'particle', 'and', 'momentum', 'balance', 'equations', 'can', 'be', 'solved', 'on', 'concentric', 'circular', 'flux', 'surfaces', 'to', 'determine', 'the', 'effective', 'viscous', 'drag', 'present', 'in', 'a', 'magnetized', 'tokamak', 'plasma', 'in', 'the', 'low', 'aspect', 'ratio', 'limit', 'an', 'analysis', ... | [-0.14272916331117425, 0.19646587528396367, -0.05289439450830996, 0.04265451995720495, -0.042253691096106445, -0.08987965637204275, -0.06594116310319847, 0.3086425194495245, -0.20370479043293205, -0.36770200431669897, 0.029363705254445188, -0.23192817548214528, -0.010504432462661856, 0.193965452434522, -0.0286826584192... |
710.2658 | Catalog of dessins d'enfants with \le 4 edges | In this work all the dessins d'enfant with no more than 4 edges are listed
and their Belyi pairs are computed. In order to enumerate all dessins the
technique of matrix model computations was used. The total number of dessins is
134; among them 77 are spherical, 53 of genus 1 and 4 of genus 2. The orders of
automorph... | math.AG | in this work all the dessins denfant with no more than 4 edges are listed and their belyi pairs are computed in order to enumerate all dessins the technique of matrix model computations was used the total number of dessins is 134 among them 77 are spherical 53 of genus 1 and 4 of genus 2 the orders of automorphism grou... | [['in', 'this', 'work', 'all', 'the', 'dessins', 'denfant', 'with', 'no', 'more', 'than', '4', 'edges', 'are', 'listed', 'and', 'their', 'belyi', 'pairs', 'are', 'computed', 'in', 'order', 'to', 'enumerate', 'all', 'dessins', 'the', 'technique', 'of', 'matrix', 'model', 'computations', 'was', 'used', 'the', 'total', 'n... | [-0.12840411288375816, 0.14685542922278597, -0.012467272409045969, 0.0905616975821313, -0.04117284555926578, -0.1262117510817888, -0.014399673416499646, 0.40130587232135634, -0.23581400516137252, -0.4068450395103174, 0.09253757030130826, -0.39213752647051375, -0.1602939207263234, 0.17174961646833947, -0.055407469662507... |
710.2659 | Rigidity and persistence for ensuring shape maintenance of multiagent
meta formations (ext'd version) | This paper treats the problem of the merging of formations, where the
underlying model of a formation is graphical. We first analyze the rigidity and
persistence of meta-formations, which are formations obtained by connecting
several rigid or persistent formations. Persistence is a generalization to
directed graphs o... | cs.MA cs.DM | this paper treats the problem of the merging of formations where the underlying model of a formation is graphical we first analyze the rigidity and persistence of metaformations which are formations obtained by connecting several rigid or persistent formations persistence is a generalization to directed graphs of the u... | [['this', 'paper', 'treats', 'the', 'problem', 'of', 'the', 'merging', 'of', 'formations', 'where', 'the', 'underlying', 'model', 'of', 'a', 'formation', 'is', 'graphical', 'we', 'first', 'analyze', 'the', 'rigidity', 'and', 'persistence', 'of', 'metaformations', 'which', 'are', 'formations', 'obtained', 'by', 'connect... | [-0.1785403408095923, 0.123486285545785, -0.08853770416400587, 0.08188420380305726, -0.07982871289016637, -0.08276695240189443, 0.021102656338155938, 0.37358826591156935, -0.3226933451689325, -0.29894688208623016, 0.12502020985982915, -0.19611413882092665, -0.16798077754406188, 0.12700802771346145, -0.06373836052113475... |
710.266 | Viscosity and confinement in magnetized plasma | An alternative to the Braginskii decomposition is proposed, one rooted in
treating the viscosity as a scalar quantity in a coordinate-free
representation. With appropriate application to the rate-of-shear tensor, one
may solve the neoclassical force density equations for its undetermined
velocity dependence, as well ... | physics.plasm-ph | an alternative to the braginskii decomposition is proposed one rooted in treating the viscosity as a scalar quantity in a coordinatefree representation with appropriate application to the rateofshear tensor one may solve the neoclassical force density equations for its undetermined velocity dependence as well as the ra... | [['an', 'alternative', 'to', 'the', 'braginskii', 'decomposition', 'is', 'proposed', 'one', 'rooted', 'in', 'treating', 'the', 'viscosity', 'as', 'a', 'scalar', 'quantity', 'in', 'a', 'coordinatefree', 'representation', 'with', 'appropriate', 'application', 'to', 'the', 'rateofshear', 'tensor', 'one', 'may', 'solve', '... | [-0.12971499898389632, 0.1431217146458775, -0.11063372703649783, 0.048392214365155686, -0.10512329838682144, -0.10895307363188338, -0.034007569361064166, 0.29612564368705663, -0.2823842671080326, -0.28541639674129704, 0.06373979544566412, -0.2578813961766187, -0.07480983062839461, 0.18230748417535944, -0.01710150128097... |
710.2661 | Affine Geometry of Space Curves | This paper is devoted to the complete classification of space curves under
affine transformations in the view of Cartan's theorem. Spivak has introduced
the method but has not found the invariants. Furthermore, for the first time,
we propound a necessary and sufficient condition for the invariants. Then, we
study the... | math.DG | this paper is devoted to the complete classification of space curves under affine transformations in the view of cartans theorem spivak has introduced the method but has not found the invariants furthermore for the first time we propound a necessary and sufficient condition for the invariants then we study the shapes o... | [['this', 'paper', 'is', 'devoted', 'to', 'the', 'complete', 'classification', 'of', 'space', 'curves', 'under', 'affine', 'transformations', 'in', 'the', 'view', 'of', 'cartans', 'theorem', 'spivak', 'has', 'introduced', 'the', 'method', 'but', 'has', 'not', 'found', 'the', 'invariants', 'furthermore', 'for', 'the', '... | [-0.1169325203734583, 0.03293575089690941, -0.13918127167437758, 0.058653046816055265, -0.07677122037857771, -0.10945360627956688, -0.01035963028968711, 0.37913511778627124, -0.2640508852100798, -0.2979091244749725, 0.11979197124518189, -0.19376582770741413, -0.22173119239243014, 0.22191797254074896, -0.169348685004349... |
710.2662 | Affine Classification of n-Curves | Classification of curves up to affine transformation in a finite dimensional
space was studied by some different methods. In this paper, we achieve the
exact formulas of affine invariants via the equivalence problem and in the view
of Cartan's lemma and then, state a necessary and sufficient condition for
classificat... | math.DG | classification of curves up to affine transformation in a finite dimensional space was studied by some different methods in this paper we achieve the exact formulas of affine invariants via the equivalence problem and in the view of cartans lemma and then state a necessary and sufficient condition for classification of... | [['classification', 'of', 'curves', 'up', 'to', 'affine', 'transformation', 'in', 'a', 'finite', 'dimensional', 'space', 'was', 'studied', 'by', 'some', 'different', 'methods', 'in', 'this', 'paper', 'we', 'achieve', 'the', 'exact', 'formulas', 'of', 'affine', 'invariants', 'via', 'the', 'equivalence', 'problem', 'and'... | [-0.09194407414864092, 0.05010394744721113, -0.09846670649872691, 0.06258693685088598, -0.06480187356618106, -0.13808812778077872, 0.07803424620115217, 0.3511136322848353, -0.3023842840875481, -0.27184180559261756, 0.14791894637678257, -0.17789362399729297, -0.1685803122088021, 0.20990771646885312, -0.1433116147444725,... |
710.2663 | A State Sum Link Invariant of Regular Isotopy | This paper has been withdrawn because there is a fundamental error in the
computations; with the right computational scheme it seems to be just a version
of the Jones polynomial
| math.GT math.CO | this paper has been withdrawn because there is a fundamental error in the computations with the right computational scheme it seems to be just a version of the jones polynomial | [['this', 'paper', 'has', 'been', 'withdrawn', 'because', 'there', 'is', 'a', 'fundamental', 'error', 'in', 'the', 'computations', 'with', 'the', 'right', 'computational', 'scheme', 'it', 'seems', 'to', 'be', 'just', 'a', 'version', 'of', 'the', 'jones', 'polynomial']] | [-0.11086263985683521, 0.015422184858471156, -0.15593986213207245, 0.009335202599565188, -0.0838366488305231, -0.1535982468165457, 0.003680686594452709, 0.3542372896025578, -0.33182427609960236, -0.30524486711559196, 0.16356546538493907, -0.2113304081062476, -0.15302882202280063, 0.17828086259153983, -0.204693470150232... |
710.2664 | Reconstructing Images from Projections Using the Maximum-Entropy Method.
Numerical Simulations of Low-Aspect Astrotomography | The reconstruction of images from a small number of projections using the
maximum-entropy method (MEM) with the Shannon entropy is considered. MEM
provides higher-quality image reconstruction for sources with extended
components than the Hogbom CLEAN method, which is also used in low-aspect
astrotomography. The quali... | astro-ph | the reconstruction of images from a small number of projections using the maximumentropy method mem with the shannon entropy is considered mem provides higherquality image reconstruction for sources with extended components than the hogbom clean method which is also used in lowaspect astrotomography the quality of imag... | [['the', 'reconstruction', 'of', 'images', 'from', 'a', 'small', 'number', 'of', 'projections', 'using', 'the', 'maximumentropy', 'method', 'mem', 'with', 'the', 'shannon', 'entropy', 'is', 'considered', 'mem', 'provides', 'higherquality', 'image', 'reconstruction', 'for', 'sources', 'with', 'extended', 'components', '... | [-0.01924115976337159, -0.002970051610528833, -0.12235450948413351, 0.06906934504139026, -0.03983363603463046, -0.11880132412574816, 0.018856694857304047, 0.3811060880670453, -0.20207449214735834, -0.31746801467483293, 0.12205999300095925, -0.26772129231381536, -0.09205152100818877, 0.25357730595607053, -0.054748506156... |
710.2665 | Lower bounds on the coefficients of Ehrhart polynomials | We present lower bounds for the coefficients of Ehrhart polynomials of convex
lattice polytopes in terms of their volume. Concerning the coefficients of the
Ehrhart series of a lattice polytope we show that Hibi's lower bound is not
true for lattice polytopes without interior lattice points. The counterexample
is bas... | math.MG math.CO | we present lower bounds for the coefficients of ehrhart polynomials of convex lattice polytopes in terms of their volume concerning the coefficients of the ehrhart series of a lattice polytope we show that hibis lower bound is not true for lattice polytopes without interior lattice points the counterexample is based on... | [['we', 'present', 'lower', 'bounds', 'for', 'the', 'coefficients', 'of', 'ehrhart', 'polynomials', 'of', 'convex', 'lattice', 'polytopes', 'in', 'terms', 'of', 'their', 'volume', 'concerning', 'the', 'coefficients', 'of', 'the', 'ehrhart', 'series', 'of', 'a', 'lattice', 'polytope', 'we', 'show', 'that', 'hibis', 'low... | [-0.1726857473491691, 0.03795410317834467, -0.1337463857140392, 0.0408341314381687, -0.10595223812852055, -0.0737312498036772, 0.10381148376327473, 0.32618724802741783, -0.32519481286872176, -0.13925211140885949, 0.1654122994383215, -0.3020013728761114, -0.20597840719856322, 0.17152479117503389, -0.1274117312626913, 0.... |
710.2666 | Generalized Chaplygin gas as geometrical dark energy | The generalized Chaplygin gas provides an interesting candidate for the
present accelerated expansion of the universe. We explore a geometrical
explanation for the generalized Chaplygin gas within the context of brane world
theories where matter fields are confined to the brane by means of the action
of a confining p... | gr-qc | the generalized chaplygin gas provides an interesting candidate for the present accelerated expansion of the universe we explore a geometrical explanation for the generalized chaplygin gas within the context of brane world theories where matter fields are confined to the brane by means of the action of a confining pote... | [['the', 'generalized', 'chaplygin', 'gas', 'provides', 'an', 'interesting', 'candidate', 'for', 'the', 'present', 'accelerated', 'expansion', 'of', 'the', 'universe', 'we', 'explore', 'a', 'geometrical', 'explanation', 'for', 'the', 'generalized', 'chaplygin', 'gas', 'within', 'the', 'context', 'of', 'brane', 'world',... | [-0.12196298451624, 0.11963509409798025, -0.12700824426825752, 0.10156704400297158, -0.10201739649856825, -0.12732992472441554, -0.0313778427405307, 0.3013468841937455, -0.21054146835556278, -0.2963354235829471, 0.037684030257854856, -0.21279545228734806, -0.0718334312369297, 0.14641141338733496, -0.03541007481043699, ... |
710.2667 | On the generalized Jacobi equation | The standard text-book Jacobi equation (equation of geodesic deviation)
arises by linearizing the geodesic equation around some chosen geodesic, where
the linearization is done with respect to the coordinates and the velocities.
The generalized Jacobi equation, introduced by Hodgkinson in 1972 and further
developed b... | gr-qc | the standard textbook jacobi equation equation of geodesic deviation arises by linearizing the geodesic equation around some chosen geodesic where the linearization is done with respect to the coordinates and the velocities the generalized jacobi equation introduced by hodgkinson in 1972 and further developed by mashho... | [['the', 'standard', 'textbook', 'jacobi', 'equation', 'equation', 'of', 'geodesic', 'deviation', 'arises', 'by', 'linearizing', 'the', 'geodesic', 'equation', 'around', 'some', 'chosen', 'geodesic', 'where', 'the', 'linearization', 'is', 'done', 'with', 'respect', 'to', 'the', 'coordinates', 'and', 'the', 'velocities'... | [-0.15455695348151938, 0.09207809939518401, -0.08691037090793821, 0.07850946217441206, -0.13885990795075098, -0.14566615972852776, -0.02355300805723394, 0.34330494098990927, -0.2534024134591108, -0.20732395934209383, 0.06200882205064231, -0.305408175586801, -0.14894820488136234, 0.15866125038050058, -0.1075795799811932... |
710.2668 | An Imaging and Spectral Study of Ten X-Ray Filaments around the Galactic
Center | We report the detection of 10 new X-ray filaments using the data from the
{\sl Chandra} X-ray satellite for the inner $6^{\prime}$ ($\sim 15$ parsec)
around the Galactic center (GC). All these X-ray filaments are characterized by
non-thermal energy spectra, and most of them have point-like features at their
heads tha... | astro-ph | we report the detection of 10 new xray filaments using the data from the sl chandra xray satellite for the inner 6prime sim 15 parsec around the galactic center gc all these xray filaments are characterized by nonthermal energy spectra and most of them have pointlike features at their heads that point inward fitted wit... | [['we', 'report', 'the', 'detection', 'of', '10', 'new', 'xray', 'filaments', 'using', 'the', 'data', 'from', 'the', 'sl', 'chandra', 'xray', 'satellite', 'for', 'the', 'inner', '6prime', 'sim', '15', 'parsec', 'around', 'the', 'galactic', 'center', 'gc', 'all', 'these', 'xray', 'filaments', 'are', 'characterized', 'by... | [-0.06049572005652623, 0.14979957578701406, -0.025226912780185743, 0.11768923209565611, -0.09797577728312785, -0.04558869246178107, 0.05080109103340548, 0.4861411777556459, -0.19900779394739754, -0.3708656169447208, 0.07239502808819337, -0.36191272932626956, 0.03183029934419373, 0.23264804230249256, 0.01919905100868358... |
710.2669 | Probing CP properties of the Higgs Boson via \boldmath{e^+e^-\to t
\bar{t}\phi | One of the main endeavors at future high-energy colliders is the search for
the Higgs boson(s) and, once found, the probe of the fundamental properties. In
particular, the charge conjugation and parity (CP) quantum numbers have to be
determined. We show that these are unambiguously accessible at future $e^+e^-$
colli... | hep-ph | one of the main endeavors at future highenergy colliders is the search for the higgs bosons and once found the probe of the fundamental properties in particular the charge conjugation and parity cp quantum numbers have to be determined we show that these are unambiguously accessible at future ee colliders through the m... | [['one', 'of', 'the', 'main', 'endeavors', 'at', 'future', 'highenergy', 'colliders', 'is', 'the', 'search', 'for', 'the', 'higgs', 'bosons', 'and', 'once', 'found', 'the', 'probe', 'of', 'the', 'fundamental', 'properties', 'in', 'particular', 'the', 'charge', 'conjugation', 'and', 'parity', 'cp', 'quantum', 'numbers',... | [-0.10424236197224153, 0.23663380171305368, -0.05861308708055211, 0.10936647771491802, -0.03061614776296275, -0.1503495822660625, 0.02552856532524207, 0.32115519350128513, -0.2732901155815593, -0.26698877695681794, 0.02166612358830337, -0.32892186168714294, 0.0020444761695606367, 0.18812191573836443, 0.1301313170631017... |
710.267 | Search for Chargino-Neutralino Pair Production at CDF | We present the results of a search for associated production of the lightest
chargino and next-to-lightest neutralino using 1 fb$^{-1}$ of $\sqrt s$ = 1.96
TeV p$\rm \bar p$ data collected with the CDF detector at the Tevatron. We
combine the results of several multi-lepton final states to set upper limits on
the cro... | hep-ex | we present the results of a search for associated production of the lightest chargino and nexttolightest neutralino using 1 fb1 of sqrt s 196 tev prm bar p data collected with the cdf detector at the tevatron we combine the results of several multilepton final states to set upper limits on the cross section times branc... | [['we', 'present', 'the', 'results', 'of', 'a', 'search', 'for', 'associated', 'production', 'of', 'the', 'lightest', 'chargino', 'and', 'nexttolightest', 'neutralino', 'using', '1', 'fb1', 'of', 'sqrt', 's', '196', 'tev', 'prm', 'bar', 'p', 'data', 'collected', 'with', 'the', 'cdf', 'detector', 'at', 'the', 'tevatron'... | [-0.060331752354369515, 0.21081066591692948, -0.0458606854498164, 0.15695334601202118, -0.004363843642953617, -0.11560335281346716, 0.07207996524529837, 0.27866136113445816, -0.17865409318413308, -0.3352781980117755, 0.0075384237553312704, -0.40954394321610676, 0.1499903842480158, 0.17834712912627398, 0.117362231252464... |
710.2671 | Sets non-thin at \infty in \Bbb C ^m, and the growth of sequences of
entire functions of genus zero | In this paper we define the notion of non-thin at $\infty$ as follows: Let
$E$ be a subset of $\Bbb C^m$. For any $R>0$ define $E_R=E\cap \{z\in \Bbb C ^m
:|z|\leq R\}$. We say that $E$ is non-thin at $\infty$ if
\lim_{R\to\infty}V_{E_R}(z)=0
for all $z\in \Bbb C^m$, where $V_E$ is the pluricomplex Green function... | math.CV math.DS | in this paper we define the notion of nonthin at infty as follows let e be a subset of bbb cm for any r0 define e_recap zin bbb c m zleq r we say that e is nonthin at infty if lim_rtoinftyv_e_rz0 for all zin bbb cm where v_e is the pluricomplex green function of e this definition of nonthin at infty has good properties... | [['in', 'this', 'paper', 'we', 'define', 'the', 'notion', 'of', 'nonthin', 'at', 'infty', 'as', 'follows', 'let', 'e', 'be', 'a', 'subset', 'of', 'bbb', 'cm', 'for', 'any', 'r0', 'define', 'e_recap', 'zin', 'bbb', 'c', 'm', 'zleq', 'r', 'we', 'say', 'that', 'e', 'is', 'nonthin', 'at', 'infty', 'if', 'lim_rtoinftyv_e_rz... | [-0.16782485522095145, 0.0705303628122302, -0.04054890986619972, -0.01074056749829773, 0.0298695190732668, -0.16992537940185018, -0.03650213493763902, 0.3459398537786223, -0.29187652220817534, -0.05377179577061632, 0.06348000775736676, -0.3902769953903456, -0.039258834806923555, 0.15497464107122183, -0.0940130107456774... |
710.2672 | A Method of Experimentally Probing Transeverse Momentum Dependent
Distributions | We calculate the double spin asymmetry A_LL(x, y, z, P_hT) of pi^0 production
with the spectator model and the model based on the factorization ansatz. We
also calculate the double spin asymmetry for the integration over the range of
(x,y,z) for the setups of the experiments of COMPASS, HERMES, and JLab. We find
that... | hep-ph | we calculate the double spin asymmetry a_llx y z p_ht of pi0 production with the spectator model and the model based on the factorization ansatz we also calculate the double spin asymmetry for the integration over the range of xyz for the setups of the experiments of compass hermes and jlab we find that the results are... | [['we', 'calculate', 'the', 'double', 'spin', 'asymmetry', 'a_llx', 'y', 'z', 'p_ht', 'of', 'pi0', 'production', 'with', 'the', 'spectator', 'model', 'and', 'the', 'model', 'based', 'on', 'the', 'factorization', 'ansatz', 'we', 'also', 'calculate', 'the', 'double', 'spin', 'asymmetry', 'for', 'the', 'integration', 'ove... | [-0.10073022577784113, 0.17293122271630204, -0.14313952455164067, 0.09543094040626394, -0.02226803213402274, -0.0999245712106737, 0.03145267329333971, 0.3639417935961059, -0.22374314706151685, -0.24343795403616414, -0.02410844444031162, -0.2921356824781036, -0.058518415316939354, 0.2263531956982444, 0.13046487949655525... |
710.2673 | Higher Derivative Corrections in M-theory via Local Supersymmetry | We investigate higher derivative corrections in M-theory by applying
Noether's method. Cancellation of variations, which contain linear terms in
4-form field strength, under local supersymmetry is executed with the aid of
computer programming. Structure of $R^4$ terms is uniquely determined and
exactly matches with o... | hep-th | we investigate higher derivative corrections in mtheory by applying noethers method cancellation of variations which contain linear terms in 4form field strength under local supersymmetry is executed with the aid of computer programming structure of r4 terms is uniquely determined and exactly matches with oneloop effec... | [['we', 'investigate', 'higher', 'derivative', 'corrections', 'in', 'mtheory', 'by', 'applying', 'noethers', 'method', 'cancellation', 'of', 'variations', 'which', 'contain', 'linear', 'terms', 'in', '4form', 'field', 'strength', 'under', 'local', 'supersymmetry', 'is', 'executed', 'with', 'the', 'aid', 'of', 'computer... | [-0.15982727999261653, 0.08066358850695766, -0.011102825481569968, 0.13067444251366675, -0.11700587959673542, -0.1360056437462425, -0.04129039447826262, 0.2813563977296536, -0.20835621850206876, -0.3339146862272173, 0.09259670251272976, -0.21860827100821412, -0.22393809703107065, 0.12007237530241792, -0.101174039013970... |
710.2674 | Linguistic Information Energy | In this treatment a text is considered to be a series of word impulses which
are read at a constant rate. The brain then assembles these units of
information into higher units of meaning. A classical systems approach is used
to model an initial part of this assembly process. The concepts of linguistic
system response... | cs.CL cs.IT math.IT | in this treatment a text is considered to be a series of word impulses which are read at a constant rate the brain then assembles these units of information into higher units of meaning a classical systems approach is used to model an initial part of this assembly process the concepts of linguistic system response info... | [['in', 'this', 'treatment', 'a', 'text', 'is', 'considered', 'to', 'be', 'a', 'series', 'of', 'word', 'impulses', 'which', 'are', 'read', 'at', 'a', 'constant', 'rate', 'the', 'brain', 'then', 'assembles', 'these', 'units', 'of', 'information', 'into', 'higher', 'units', 'of', 'meaning', 'a', 'classical', 'systems', '... | [-0.10241745491512119, 0.07636328676550572, -0.10101260243164789, 0.09550253422876268, -0.0836382655840781, -0.07058456955581076, 0.06548325396660301, 0.3566226351178355, -0.32086474363588624, -0.31690529037991333, 0.10982851294490198, -0.3023532697723971, -0.12840259001499765, 0.17274776980436096, -0.05440647144957135... |
710.2675 | Band Gap of CsCl Film's as a Function of Lattice Constant | The manuscript reports experimental estimation of Cesium Chloride film's band
gap and compares it with theoretical simulations. The band gap shows a strong
dependence on it's lattice constant. Also, it is seen that the point defects
present in the films strongly affects it's optical properties.
| cond-mat.mtrl-sci | the manuscript reports experimental estimation of cesium chloride films band gap and compares it with theoretical simulations the band gap shows a strong dependence on its lattice constant also it is seen that the point defects present in the films strongly affects its optical properties | [['the', 'manuscript', 'reports', 'experimental', 'estimation', 'of', 'cesium', 'chloride', 'films', 'band', 'gap', 'and', 'compares', 'it', 'with', 'theoretical', 'simulations', 'the', 'band', 'gap', 'shows', 'a', 'strong', 'dependence', 'on', 'its', 'lattice', 'constant', 'also', 'it', 'is', 'seen', 'that', 'the', 'p... | [-0.13836908902352055, 0.09821845699205167, -0.06716360420816475, -0.03304159790277481, -0.02054940385537015, -0.10971195388378369, 0.12438479497925276, 0.5143373214536243, -0.25997675048808255, -0.2737858416305648, 0.0587852085293788, -0.35020671834548317, -0.1632613154542115, 0.1585802318321334, -0.012635345777703656... |
710.2676 | Radiation Damage Study for PHENIX Silicon Stripixel Sensors | Silicon stripixel sensors which were developed at BNL will be installed as
part of the RHIC-PHENIX silicon vertex tracker (VTX). RHIC II operations
provide luminosity up to 2x10^32 /cm2/s so the silicon stripixel sensors will
be exposed to a significant amount of radiation. The most problematic radiation
effect for V... | nucl-ex | silicon stripixel sensors which were developed at bnl will be installed as part of the rhicphenix silicon vertex tracker vtx rhic ii operations provide luminosity up to 2x1032 cm2s so the silicon stripixel sensors will be exposed to a significant amount of radiation the most problematic radiation effect for vtx is the ... | [['silicon', 'stripixel', 'sensors', 'which', 'were', 'developed', 'at', 'bnl', 'will', 'be', 'installed', 'as', 'part', 'of', 'the', 'rhicphenix', 'silicon', 'vertex', 'tracker', 'vtx', 'rhic', 'ii', 'operations', 'provide', 'luminosity', 'up', 'to', '2x1032', 'cm2s', 'so', 'the', 'silicon', 'stripixel', 'sensors', 'w... | [-0.0544750558761641, 0.1619895483749226, -0.02378608373662409, 0.0207871710941291, -0.011128525350702544, -0.15447734458228715, 0.01611227315181914, 0.3947846826667396, -0.22338470836611798, -0.37830133101640223, 0.06933739783648306, -0.3697572657575783, 0.03376532417889207, 0.20138379010634544, -0.07335482763547378, ... |
710.2677 | The scalar unparticle effect on the charged lepton electric dipole
moment | We study the charged lepton electric dipole moment which is induced by the
scalar unparticle mediation and we predict the appropriate range for the free
parameters appearing in the effective lagrangian which drives the
unparticle-standard model lepton interactions. We observe that the charged
lepton electric dipole m... | hep-ph | we study the charged lepton electric dipole moment which is induced by the scalar unparticle mediation and we predict the appropriate range for the free parameters appearing in the effective lagrangian which drives the unparticlestandard model lepton interactions we observe that the charged lepton electric dipole momen... | [['we', 'study', 'the', 'charged', 'lepton', 'electric', 'dipole', 'moment', 'which', 'is', 'induced', 'by', 'the', 'scalar', 'unparticle', 'mediation', 'and', 'we', 'predict', 'the', 'appropriate', 'range', 'for', 'the', 'free', 'parameters', 'appearing', 'in', 'the', 'effective', 'lagrangian', 'which', 'drives', 'the... | [-0.13846926307252777, 0.3046731385364348, 0.020730532511978792, 0.152777217870938, -0.09321532098428262, -0.11293532780837268, -0.005731523453670723, 0.3085305208170956, -0.22006247956729072, -0.32929489069448953, -0.05227623573260975, -0.28811197814700956, -0.07808537664823234, 0.07715419463718055, 0.0942371923434124... |
710.2678 | Adaptive Directional Subdivision Schemes and Shearlet Multiresolution
Analysis | In this paper, we propose a solution for a fundamental problem in
computational harmonic analysis, namely, the construction of a multiresolution
analysis with directional components. We will do so by constructing subdivision
schemes which provide a means to incorporate directionality into the data and
thus the limit ... | math.NA math.FA | in this paper we propose a solution for a fundamental problem in computational harmonic analysis namely the construction of a multiresolution analysis with directional components we will do so by constructing subdivision schemes which provide a means to incorporate directionality into the data and thus the limit functi... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'solution', 'for', 'a', 'fundamental', 'problem', 'in', 'computational', 'harmonic', 'analysis', 'namely', 'the', 'construction', 'of', 'a', 'multiresolution', 'analysis', 'with', 'directional', 'components', 'we', 'will', 'do', 'so', 'by', 'constructing', 'subdivision', '... | [-0.08241491052213389, 0.01498353462217443, -0.13669334800846605, 0.03279075214219799, -0.12886515028314688, -0.1229250800391906, 0.04396083419623571, 0.429128588850509, -0.2866959431340514, -0.22362130174009376, 0.13123820233719805, -0.18088198432990585, -0.24375188228231012, 0.1998997710284732, -0.1017440599445478, 0... |
710.2679 | A New Class of Group Field Theories for 1st Order Discrete Quantum
Gravity | Group Field Theories, a generalization of matrix models for 2d gravity,
represent a 2nd quantization of both loop quantum gravity and simplicial
quantum gravity. In this paper, we construct a new class of Group Field Theory
models, for any choice of spacetime dimension and signature, whose Feynman
amplitudes are give... | gr-qc hep-th | group field theories a generalization of matrix models for 2d gravity represent a 2nd quantization of both loop quantum gravity and simplicial quantum gravity in this paper we construct a new class of group field theory models for any choice of spacetime dimension and signature whose feynman amplitudes are given by pat... | [['group', 'field', 'theories', 'a', 'generalization', 'of', 'matrix', 'models', 'for', '2d', 'gravity', 'represent', 'a', '2nd', 'quantization', 'of', 'both', 'loop', 'quantum', 'gravity', 'and', 'simplicial', 'quantum', 'gravity', 'in', 'this', 'paper', 'we', 'construct', 'a', 'new', 'class', 'of', 'group', 'field', ... | [-0.12272467937380556, 0.1601100701764564, -0.11274406288059488, 0.10203493283385591, -0.11850777518364691, -0.16574531589304248, -0.01322500850524633, 0.2961709147018771, -0.22870550280016277, -0.28037815977849306, 0.061310043516418625, -0.21939136454414937, -0.18731441264221024, 0.16336223815733025, -0.10973600163575... |
710.268 | Global properties of Stochastic Loewner evolution driven by Levy
processes | Standard Schramm-Loewner evolution (SLE) is driven by a continuous Brownian
motion which then produces a trace, a continuous fractal curve connecting the
singular points of the motion. If jumps are added to the driving function, the
trace branches. In a recent publication [1] we introduced a generalized SLE
driven by... | cond-mat.stat-mech | standard schrammloewner evolution sle is driven by a continuous brownian motion which then produces a trace a continuous fractal curve connecting the singular points of the motion if jumps are added to the driving function the trace branches in a recent publication 1 we introduced a generalized sle driven by a superpos... | [['standard', 'schrammloewner', 'evolution', 'sle', 'is', 'driven', 'by', 'a', 'continuous', 'brownian', 'motion', 'which', 'then', 'produces', 'a', 'trace', 'a', 'continuous', 'fractal', 'curve', 'connecting', 'the', 'singular', 'points', 'of', 'the', 'motion', 'if', 'jumps', 'are', 'added', 'to', 'the', 'driving', 'f... | [-0.11681500960504777, 0.18323668520536035, -0.09260785411937501, 0.058141179522470506, -0.019781845966600955, -0.13264350776355996, 0.020302805577750514, 0.33541038090708863, -0.32132287054484937, -0.2211682120541809, 0.08587637021529107, -0.2839803669657241, -0.11866290942116668, 0.18531905807410085, -0.0158294428732... |
710.2681 | Multiplicative properties of Morin maps | In the first part of the paper we construct a ring structure on the rational
cobordism classes of Morin maps (i. e. smooth generic maps of corank 1). We
show that associating to a Morin map its singular strata defines a ring
homomorphism to $\Omega_* \otimes \Q$, the rational oriented cobordism ring.
This is proved b... | math.GT math.AT | in the first part of the paper we construct a ring structure on the rational cobordism classes of morin maps i e smooth generic maps of corank 1 we show that associating to a morin map its singular strata defines a ring homomorphism to omega_ otimes q the rational oriented cobordism ring this is proved by analyzing mul... | [['in', 'the', 'first', 'part', 'of', 'the', 'paper', 'we', 'construct', 'a', 'ring', 'structure', 'on', 'the', 'rational', 'cobordism', 'classes', 'of', 'morin', 'maps', 'i', 'e', 'smooth', 'generic', 'maps', 'of', 'corank', '1', 'we', 'show', 'that', 'associating', 'to', 'a', 'morin', 'map', 'its', 'singular', 'strat... | [-0.22333054772552546, -0.009669690290380508, -0.09788535390083396, 0.03188461514719582, -0.055764012628260556, -0.13708516641374713, -0.059864437995786106, 0.32218864370445044, -0.3664278953652316, -0.14452238595369485, 0.07762435626093332, -0.27347197578450955, -0.17882470751967317, 0.14943079023254574, -0.1119073017... |
710.2682 | Cuspidal representations of sl(n+1) | In this paper we study the subcategory of cuspidal modules of the category of
weight modules over the Lie algebra sl(n+1). Our main result is a complete
classification and explicit description of the indecomposable cuspidal modules.
| math.RT | in this paper we study the subcategory of cuspidal modules of the category of weight modules over the lie algebra sln1 our main result is a complete classification and explicit description of the indecomposable cuspidal modules | [['in', 'this', 'paper', 'we', 'study', 'the', 'subcategory', 'of', 'cuspidal', 'modules', 'of', 'the', 'category', 'of', 'weight', 'modules', 'over', 'the', 'lie', 'algebra', 'sln1', 'our', 'main', 'result', 'is', 'a', 'complete', 'classification', 'and', 'explicit', 'description', 'of', 'the', 'indecomposable', 'cusp... | [-0.22228679747786373, -0.07671394232764012, -0.09496339827051593, -0.006482374440464709, -0.11097586817211574, -0.061433298034696944, -0.0819714832759928, 0.35008450266387725, -0.39153748989984805, -0.17119394752403927, 0.08465184809109713, -0.16692089249328193, -0.16850844389894823, 0.17746312665339145, -0.2218522971... |
710.2683 | On the dynamics of a twisted disc immersed in a radiation field | We study the dynamics of a twisted tilted disc under the influence of an
external radiation field. Assuming the effect of absorption and
reemission/scattering is that a pressure is applied to the disc surface where
the local optical depth is of order unity, we determine the response of the
vertical structure and the ... | astro-ph | we study the dynamics of a twisted tilted disc under the influence of an external radiation field assuming the effect of absorption and reemissionscattering is that a pressure is applied to the disc surface where the local optical depth is of order unity we determine the response of the vertical structure and the influ... | [['we', 'study', 'the', 'dynamics', 'of', 'a', 'twisted', 'tilted', 'disc', 'under', 'the', 'influence', 'of', 'an', 'external', 'radiation', 'field', 'assuming', 'the', 'effect', 'of', 'absorption', 'and', 'reemissionscattering', 'is', 'that', 'a', 'pressure', 'is', 'applied', 'to', 'the', 'disc', 'surface', 'where', ... | [-0.15295075099274003, 0.15628825863038373, -0.07645015555297915, 0.04862518169366839, -0.07555627046852226, -0.062252684165911766, -0.00831219067433316, 0.3623577481831866, -0.298440163491783, -0.2678933798787043, 0.078199809357549, -0.23958350413852067, -0.09031848372775522, 0.16898582953809185, -0.008931733856535428... |
710.2684 | Open charm in nuclear matter at finite temperature | We study the properties of open-charm mesons ($D$ and $\bar {D}$) in nuclear
matter at finite temperature within a self-consistent coupled-channel approach.
The meson-baryon interactions are adopted from a type of broken SU(4) s-wave
Tomozawa-Weinberg terms supplemented by an attractive scalar-isoscalar
attraction. T... | nucl-th hep-ph | we study the properties of opencharm mesons d and bar d in nuclear matter at finite temperature within a selfconsistent coupledchannel approach the mesonbaryon interactions are adopted from a type of broken su4 swave tomozawaweinberg terms supplemented by an attractive scalarisoscalar attraction the inmedium solution a... | [['we', 'study', 'the', 'properties', 'of', 'opencharm', 'mesons', 'd', 'and', 'bar', 'd', 'in', 'nuclear', 'matter', 'at', 'finite', 'temperature', 'within', 'a', 'selfconsistent', 'coupledchannel', 'approach', 'the', 'mesonbaryon', 'interactions', 'are', 'adopted', 'from', 'a', 'type', 'of', 'broken', 'su4', 'swave',... | [-0.11193718421635787, 0.2201965416838804, -0.09974242299034168, 0.12886984960339334, -0.00404205596154088, -0.12561489448850385, 0.08214884189066368, 0.3175037374953816, -0.21508355394864528, -0.244009115924712, -0.06515701682391492, -0.3331705551308245, -0.029717211822729187, 0.08209856019407769, 0.08392494697518212,... |
710.2685 | The Three Hat Problem | In this paper we study the Three Hat Problem which appeared in Puzzle Corner
of the Technology Review magazine. This puzzle gives a scenario in which three
players wearing hats are sitting together and each hat can be seen by everyone
except the player that is wearing that hat. Each player is told that all of the
hat... | math.HO | in this paper we study the three hat problem which appeared in puzzle corner of the technology review magazine this puzzle gives a scenario in which three players wearing hats are sitting together and each hat can be seen by everyone except the player that is wearing that hat each player is told that all of the hats co... | [['in', 'this', 'paper', 'we', 'study', 'the', 'three', 'hat', 'problem', 'which', 'appeared', 'in', 'puzzle', 'corner', 'of', 'the', 'technology', 'review', 'magazine', 'this', 'puzzle', 'gives', 'a', 'scenario', 'in', 'which', 'three', 'players', 'wearing', 'hats', 'are', 'sitting', 'together', 'and', 'each', 'hat', ... | [-0.11474579055793584, 0.11542025516500871, -0.13072515572227228, 0.034601081014261584, -0.12189319112803787, -0.29044293860982484, 0.0532240145461401, 0.35501176794059575, -0.2709707752762673, -0.2840949572312335, 0.09663396590622142, -0.3358534840033826, -0.1649473777913954, 0.0863686404171555, -0.12917285108705984, ... |
710.2686 | Mean first passage time for a Markovian jumping process | We consider a Markovian jumping process with two absorbing barriers, for
which the waiting-time distribution involves a position-dependent coefficient.
We solve the Fokker-Planck equation with boundary conditions and calculate the
mean first passage time (MFPT) which appears always finite, also for the
subdiffusive c... | cond-mat.stat-mech | we consider a markovian jumping process with two absorbing barriers for which the waitingtime distribution involves a positiondependent coefficient we solve the fokkerplanck equation with boundary conditions and calculate the mean first passage time mfpt which appears always finite also for the subdiffusive case then f... | [['we', 'consider', 'a', 'markovian', 'jumping', 'process', 'with', 'two', 'absorbing', 'barriers', 'for', 'which', 'the', 'waitingtime', 'distribution', 'involves', 'a', 'positiondependent', 'coefficient', 'we', 'solve', 'the', 'fokkerplanck', 'equation', 'with', 'boundary', 'conditions', 'and', 'calculate', 'the', 'm... | [-0.07166351500969519, 0.150994497945468, -0.11883625453445075, 0.07682101712476003, -0.006111787387234126, -0.11328034690613377, 0.03523828714400872, 0.3932724504720891, -0.2704259584411636, -0.24516013365281725, 0.08671196416186319, -0.2596994711557168, -0.13096253606009073, 0.17735936707849131, 0.0040650928510759755... |
710.2687 | Logarithmic tensor product theory for generalized modules for a
conformal vertex algebra | We generalize the tensor product theory for modules for a vertex operator
algebra previously developed in a series of papers by the first two authors to
suitable module categories for a ''conformal vertex algebra'' or even more
generally, for a "M\"obius vertex algebra.'' We do not require the module
categories to be... | math.QA hep-th math.RT | we generalize the tensor product theory for modules for a vertex operator algebra previously developed in a series of papers by the first two authors to suitable module categories for a conformal vertex algebra or even more generally for a mobius vertex algebra we do not require the module categories to be semisimple a... | [['we', 'generalize', 'the', 'tensor', 'product', 'theory', 'for', 'modules', 'for', 'a', 'vertex', 'operator', 'algebra', 'previously', 'developed', 'in', 'a', 'series', 'of', 'papers', 'by', 'the', 'first', 'two', 'authors', 'to', 'suitable', 'module', 'categories', 'for', 'a', 'conformal', 'vertex', 'algebra', 'or',... | [-0.11655176063298552, 0.0427120116086089, -0.07385272477917812, 0.047067216069581995, -0.1438982687046363, -0.07946754960507593, -0.020114090579703828, 0.34173853334816384, -0.3280006151790805, -0.23340818586256257, 0.11042332340076685, -0.2143231954495298, -0.17504120345307106, 0.13103684602133472, -0.115012680509072... |
710.2688 | On the invariant thermal Proca - Klein - Gordon equation | In this paper we discuss the invariant thermal Proca - Klein - Gordon
equation (PKG). We argue that for the thermal PKG equation the absolute
velocity is equal v = alpha*c, where alpha is the fine stucture constant for
electromagnetic interaction.
| physics.gen-ph | in this paper we discuss the invariant thermal proca klein gordon equation pkg we argue that for the thermal pkg equation the absolute velocity is equal v alphac where alpha is the fine stucture constant for electromagnetic interaction | [['in', 'this', 'paper', 'we', 'discuss', 'the', 'invariant', 'thermal', 'proca', 'klein', 'gordon', 'equation', 'pkg', 'we', 'argue', 'that', 'for', 'the', 'thermal', 'pkg', 'equation', 'the', 'absolute', 'velocity', 'is', 'equal', 'v', 'alphac', 'where', 'alpha', 'is', 'the', 'fine', 'stucture', 'constant', 'for', 'e... | [-0.1923754441944, 0.18133798315140762, -0.06424729354483516, 0.07947501776997294, -0.14227782345474943, -0.14379112564615512, -0.023664552764354373, 0.32791653187259245, -0.26057805385636656, -0.27435983050810664, -0.007929745880813388, -0.28435137027286383, -0.13722886679399954, 0.14781093107242332, 0.003895058100552... |
710.2689 | Evanescent states in 2D electron systems with spin-orbit interaction and
spin-dependent transmission through a barrier | We find that the total spectrum of electron states in a bounded 2D electron
gas with spin-orbit interaction contains two types of evanescent states lying
in different energy ranges. The first-type states fill in a gap, which opens in
the band of propagating spin-splitted states if tangential momentum is nonzero.
They... | cond-mat.mes-hall | we find that the total spectrum of electron states in a bounded 2d electron gas with spinorbit interaction contains two types of evanescent states lying in different energy ranges the firsttype states fill in a gap which opens in the band of propagating spinsplitted states if tangential momentum is nonzero they are des... | [['we', 'find', 'that', 'the', 'total', 'spectrum', 'of', 'electron', 'states', 'in', 'a', 'bounded', '2d', 'electron', 'gas', 'with', 'spinorbit', 'interaction', 'contains', 'two', 'types', 'of', 'evanescent', 'states', 'lying', 'in', 'different', 'energy', 'ranges', 'the', 'firsttype', 'states', 'fill', 'in', 'a', 'g... | [-0.19607713763052115, 0.2330630816606739, -0.044905056462398375, 0.05649161551431378, -0.042706156277964855, -0.13395475101892718, 0.002941466118583734, 0.39737737546514335, -0.28500945797730665, -0.2927977807766988, -0.03632648636910786, -0.3197473644509098, -0.04886069820307987, 0.1752061404972926, 0.057887999273986... |
710.269 | Another introduction to the geometry of metric spaces | Here Lipschitz conditions are used as a primary tool, for studying curves in
metric spaces in particular.
| math.MG | here lipschitz conditions are used as a primary tool for studying curves in metric spaces in particular | [['here', 'lipschitz', 'conditions', 'are', 'used', 'as', 'a', 'primary', 'tool', 'for', 'studying', 'curves', 'in', 'metric', 'spaces', 'in', 'particular']] | [-0.07541785383706584, 0.09895005196278148, -0.13785654755637927, 0.210702009334722, -0.06339797135168578, -0.13571022656362722, -0.0734148753039977, 0.4449707423062885, -0.2668759467847207, -0.2063232649336843, 0.18305501608890207, -0.18726244768785202, -0.20992273903068373, 0.3592665103428504, -0.15125710048767574, 0... |
710.2691 | V1647 Orionis: One Year into Quiescence | We present new optical, near-IR, and mid-IR observations of the young
eruptive variable star V1647 Orionis that went into outburst in late 2004 for
approximately two years. Our observations were taken one year after the star
had faded to its pre-outburst optical brightness and show that V1647Ori is
still actively acc... | astro-ph | we present new optical nearir and midir observations of the young eruptive variable star v1647 orionis that went into outburst in late 2004 for approximately two years our observations were taken one year after the star had faded to its preoutburst optical brightness and show that v1647ori is still actively accreting c... | [['we', 'present', 'new', 'optical', 'nearir', 'and', 'midir', 'observations', 'of', 'the', 'young', 'eruptive', 'variable', 'star', 'v1647', 'orionis', 'that', 'went', 'into', 'outburst', 'in', 'late', '2004', 'for', 'approximately', 'two', 'years', 'our', 'observations', 'were', 'taken', 'one', 'year', 'after', 'the'... | [0.025115184690434323, 0.079621276213874, -0.06519471081177312, 0.07121108125200587, -0.1319541204364492, -0.12818371329476924, 0.06258537009920762, 0.49216331889639137, -0.1676408082318029, -0.33828792851316475, 0.11778357464570777, -0.3057516880557348, -0.031037382297077892, 0.18630519059176245, -0.08768286644522671,... |
710.2692 | Nanomorphology of the blue iridescent wings of a giant tropical wasp,
"Megascolia procer javanensis" (Hymenoptera) | The wings of the giant wasp "Megascolia Procer Javanensis" are opaque and
iridescent. The origin of the blue-green iridescence is studied in detail,
using reflection spectroscopy, scanning electron microscopy and physical
modelling. It is shown that the structure responsible for the iridescence is a
single homogeneou... | physics.optics cond-mat.soft physics.bio-ph | the wings of the giant wasp megascolia procer javanensis are opaque and iridescent the origin of the bluegreen iridescence is studied in detail using reflection spectroscopy scanning electron microscopy and physical modelling it is shown that the structure responsible for the iridescence is a single homogeneous transpa... | [['the', 'wings', 'of', 'the', 'giant', 'wasp', 'megascolia', 'procer', 'javanensis', 'are', 'opaque', 'and', 'iridescent', 'the', 'origin', 'of', 'the', 'bluegreen', 'iridescence', 'is', 'studied', 'in', 'detail', 'using', 'reflection', 'spectroscopy', 'scanning', 'electron', 'microscopy', 'and', 'physical', 'modellin... | [-0.10479642817090887, 0.13542836135874192, -0.07277819090988487, 0.011046022058775027, -0.0735435997818907, -0.09172591638440887, 0.00189068947530662, 0.3987272729724646, -0.2624937648822864, -0.24938023338094353, 0.08589827300670247, -0.26537724696099757, -0.14705145282670856, 0.17386879118159412, -0.0096334133793910... |
710.2693 | Large-scale horizontal flows in the solar photosphere II: Long-term
behaviour and magnetic activity response | Recently, we have developed a method useful for mapping large-scale
horizontal velocity fields in the solar photosphere. The method was developed,
tuned and calibrated using the synthetic data. Now, we applied the method to
the series of Michelson Doppler Imager (MDI) dopplergrams covering almost one
solar cycle in o... | astro-ph | recently we have developed a method useful for mapping largescale horizontal velocity fields in the solar photosphere the method was developed tuned and calibrated using the synthetic data now we applied the method to the series of michelson doppler imager mdi dopplergrams covering almost one solar cycle in order to ge... | [['recently', 'we', 'have', 'developed', 'a', 'method', 'useful', 'for', 'mapping', 'largescale', 'horizontal', 'velocity', 'fields', 'in', 'the', 'solar', 'photosphere', 'the', 'method', 'was', 'developed', 'tuned', 'and', 'calibrated', 'using', 'the', 'synthetic', 'data', 'now', 'we', 'applied', 'the', 'method', 'to'... | [-0.14567899902235346, 0.16684455015029714, -0.07105398932225608, 0.0775574125386461, -0.05111404663945835, -0.04107668998095995, 0.019366103243485738, 0.396029208213664, -0.25688926425601283, -0.3418034362436559, 0.09560822915955214, -0.23603256993472035, -0.14842864369543698, 0.25649578992180555, -0.03084440838770556... |
710.2694 | Modeling Wildland Fire Propagation with Level Set Methods | Level set methods are versatile and extensible techniques for general front
tracking problems, including the practically important problem of predicting
the advance of a firefront across expanses of surface vegetation. Given a rule,
empirical or otherwise, to specify the rate of advance of an infinitesimal
segment of... | math.NA | level set methods are versatile and extensible techniques for general front tracking problems including the practically important problem of predicting the advance of a firefront across expanses of surface vegetation given a rule empirical or otherwise to specify the rate of advance of an infinitesimal segment of firef... | [['level', 'set', 'methods', 'are', 'versatile', 'and', 'extensible', 'techniques', 'for', 'general', 'front', 'tracking', 'problems', 'including', 'the', 'practically', 'important', 'problem', 'of', 'predicting', 'the', 'advance', 'of', 'a', 'firefront', 'across', 'expanses', 'of', 'surface', 'vegetation', 'given', 'a... | [-0.0813767290887386, 0.04940383293325056, -0.05727697396535648, 0.05300483613224276, -0.08481969688050818, -0.1161546063307433, 0.04823593472880957, 0.3484314018261093, -0.28765857778950643, -0.30113125845126, 0.1256112115634006, -0.2557046537974499, -0.14620791486404505, 0.2449085511910351, -0.08027084558074925, 0.09... |
710.2695 | Optical structure and function of the white filamentary hair covering
the edelweiss bracts | The optical properties of the inflorescence of the high-altitude
''Leontopodium nivale'' subsp. ''alpinum'' (edelweiss) is investigated, in
relation with its submicrometer structure, as determined by scanning electron
microscopy. The filaments forming the hair layer have been found to exhibit an
internal structure wh... | physics.optics cond-mat.soft physics.bio-ph | the optical properties of the inflorescence of the highaltitude leontopodium nivale subsp alpinum edelweiss is investigated in relation with its submicrometer structure as determined by scanning electron microscopy the filaments forming the hair layer have been found to exhibit an internal structure which may be one of... | [['the', 'optical', 'properties', 'of', 'the', 'inflorescence', 'of', 'the', 'highaltitude', 'leontopodium', 'nivale', 'subsp', 'alpinum', 'edelweiss', 'is', 'investigated', 'in', 'relation', 'with', 'its', 'submicrometer', 'structure', 'as', 'determined', 'by', 'scanning', 'electron', 'microscopy', 'the', 'filaments',... | [-0.10724256321166953, 0.12908320517315242, -0.0889142880482333, -0.013069785057034876, -0.04096652585126105, -0.11988704184602414, 0.025454705026155957, 0.4090442466239134, -0.26084522940218446, -0.3052646777636948, 0.074515210506728, -0.30465509375512956, -0.14340888659159343, 0.20378937978918354, -0.0030745184581194... |
710.2696 | Time Machine at the LHC | Recently, black hole and brane production at CERN's Large Hadron Collider
(LHC) has been widely discussed. We suggest that there is a possibility to test
causality at the LHC. We argue that if the scale of quantum gravity is of the
order of few TeVs, proton-proton collisions at the LHC could lead to the
formation of ... | hep-ph gr-qc hep-th | recently black hole and brane production at cerns large hadron collider lhc has been widely discussed we suggest that there is a possibility to test causality at the lhc we argue that if the scale of quantum gravity is of the order of few tevs protonproton collisions at the lhc could lead to the formation of time machi... | [['recently', 'black', 'hole', 'and', 'brane', 'production', 'at', 'cerns', 'large', 'hadron', 'collider', 'lhc', 'has', 'been', 'widely', 'discussed', 'we', 'suggest', 'that', 'there', 'is', 'a', 'possibility', 'to', 'test', 'causality', 'at', 'the', 'lhc', 'we', 'argue', 'that', 'if', 'the', 'scale', 'of', 'quantum',... | [-0.1337890438819237, 0.18316311055298964, -0.13622049881788573, 0.18110532090553624, -0.09089288783507596, -0.17394578351853615, -0.052744048468353184, 0.28621481918468533, -0.1842068774330852, -0.2817766039344154, 0.04387691305956984, -0.33759643595746097, 0.03316525958491851, 0.15614830094671026, 0.03024358117430330... |
710.2697 | Ly Alpha-Emitting Galaxies at z=3.1: L* Progenitors Experiencing Rapid
Star Formation | We studied the clustering properties and multiwavelength spectral energy
distributions of a complete sample of 162 Ly Alpha-Emitting (LAE) galaxies at
z=3.1 discovered in deep narrow-band MUSYC imaging of the Extended Chandra Deep
Field South. LAEs were selected to have observed frame equivalent widths >80A
and emiss... | astro-ph | we studied the clustering properties and multiwavelength spectral energy distributions of a complete sample of 162 ly alphaemitting lae galaxies at z31 discovered in deep narrowband musyc imaging of the extended chandra deep field south laes were selected to have observed frame equivalent widths 80a and emission line f... | [['we', 'studied', 'the', 'clustering', 'properties', 'and', 'multiwavelength', 'spectral', 'energy', 'distributions', 'of', 'a', 'complete', 'sample', 'of', '162', 'ly', 'alphaemitting', 'lae', 'galaxies', 'at', 'z31', 'discovered', 'in', 'deep', 'narrowband', 'musyc', 'imaging', 'of', 'the', 'extended', 'chandra', 'd... | [-0.0349881140602145, 0.10259812082565697, -0.06239134894335211, 0.1544985075565175, -0.119384353704123, -0.054997622009462684, 0.028235363703053205, 0.481718163625557, -0.03798189120369168, -0.4234881536923189, -0.03094268470548909, -0.282051464131046, 0.05546798732315586, 0.15304033270069745, 0.013519152287441773, -0... |
710.2698 | Photon storage in Lambda-type optically dense atomic media. IV. Optimal
control using gradient ascent | We use the numerical gradient ascent method from optimal control theory to
extend efficient photon storage in Lambda-type media to previously inaccessible
regimes and to provide simple intuitive explanations for our optimization
techniques. In particular, by using gradient ascent to shape classical control
pulses use... | quant-ph | we use the numerical gradient ascent method from optimal control theory to extend efficient photon storage in lambdatype media to previously inaccessible regimes and to provide simple intuitive explanations for our optimization techniques in particular by using gradient ascent to shape classical control pulses used to ... | [['we', 'use', 'the', 'numerical', 'gradient', 'ascent', 'method', 'from', 'optimal', 'control', 'theory', 'to', 'extend', 'efficient', 'photon', 'storage', 'in', 'lambdatype', 'media', 'to', 'previously', 'inaccessible', 'regimes', 'and', 'to', 'provide', 'simple', 'intuitive', 'explanations', 'for', 'our', 'optimizat... | [-0.10490985579090192, 0.11491923302443562, -0.09213799905652802, 0.07386802586552221, -0.0712324924301356, -0.13589345962585261, 0.09934457789931912, 0.4519424316570318, -0.32235361393541095, -0.3259070827548082, 0.06695631624024827, -0.20717333858289447, -0.1303751075679126, 0.22698519072243167, -0.09413749319695247,... |
710.2699 | Lower bounds for warping functions on warped-product AHE manifolds | Let $[\gamma]$ be the conformal boundary of a warped product $C^{3,\alpha}$
AHE metric $g=g_M+u^2h$ on $N=M \times F$, where $(F,h)$ is compact with unit
volume and nonpositive curvature. We show that if $[\gamma]$ has positive
Yamabe constant, then $u$ has a positive lower bound that depends only on
$[\gamma]$.
| math.DG | let gamma be the conformal boundary of a warped product c3alpha ahe metric gg_mu2h on nm times f where fh is compact with unit volume and nonpositive curvature we show that if gamma has positive yamabe constant then u has a positive lower bound that depends only on gamma | [['let', 'gamma', 'be', 'the', 'conformal', 'boundary', 'of', 'a', 'warped', 'product', 'c3alpha', 'ahe', 'metric', 'gg_mu2h', 'on', 'nm', 'times', 'f', 'where', 'fh', 'is', 'compact', 'with', 'unit', 'volume', 'and', 'nonpositive', 'curvature', 'we', 'show', 'that', 'if', 'gamma', 'has', 'positive', 'yamabe', 'constan... | [-0.20063444560704133, 0.19778156497341115, -0.06303944694809616, -0.05363746651710244, -0.13420779588826312, -0.24806824918293083, -0.02470740528466801, 0.3805945554437737, -0.21902069453305253, -0.15357845389128974, 0.11630995900486596, -0.3234424255788326, -0.11908434703946114, 0.1892420130316168, -0.063979684627459... |
710.27 | Percolative Effects on Noise in Pentacene Transistors | The 1/f noise in pentacene thin film transistors has been measured as a
function of device thickness from well above the effective conduction channel
thickness to only two conducting layers. Over the entire thickness range, the
spectral noise form is 1/f, and the noise parameter varies as (gate voltage)-1,
confirming... | cond-mat.mtrl-sci cond-mat.dis-nn | the 1f noise in pentacene thin film transistors has been measured as a function of device thickness from well above the effective conduction channel thickness to only two conducting layers over the entire thickness range the spectral noise form is 1f and the noise parameter varies as gate voltage1 confirming that the n... | [['the', '1f', 'noise', 'in', 'pentacene', 'thin', 'film', 'transistors', 'has', 'been', 'measured', 'as', 'a', 'function', 'of', 'device', 'thickness', 'from', 'well', 'above', 'the', 'effective', 'conduction', 'channel', 'thickness', 'to', 'only', 'two', 'conducting', 'layers', 'over', 'the', 'entire', 'thickness', '... | [-0.1319544914330603, 0.1602830592632277, 0.007660056376468619, 0.004671295593986858, 0.007422856390191128, -0.12343829192164145, 0.03593301698945615, 0.41776492218581995, -0.31277913909063354, -0.34925344088399896, 0.05290761817251427, -0.3004900767867054, -0.10381552599826638, 0.2155231614121977, -0.06380922972623791... |
710.2701 | Chaotic quantum dots with strongly correlated electrons | Quantum dots pose a problem where one must confront three obstacles:
randomness, interactions and finite size. Yet it is this confluence that allows
one to make some theoretical advances by invoking three theoretical tools:
Random Matrix theory (RMT), the Renormalization Group (RG) and the 1/N
expansion. Here the rea... | cond-mat.mes-hall | quantum dots pose a problem where one must confront three obstacles randomness interactions and finite size yet it is this confluence that allows one to make some theoretical advances by invoking three theoretical tools random matrix theory rmt the renormalization group rg and the 1n expansion here the reader is introd... | [['quantum', 'dots', 'pose', 'a', 'problem', 'where', 'one', 'must', 'confront', 'three', 'obstacles', 'randomness', 'interactions', 'and', 'finite', 'size', 'yet', 'it', 'is', 'this', 'confluence', 'that', 'allows', 'one', 'to', 'make', 'some', 'theoretical', 'advances', 'by', 'invoking', 'three', 'theoretical', 'tool... | [-0.08729703141815803, 0.15457674215587092, -0.13352350321103176, 0.08720643375836261, -0.10589759385633007, -0.20680650481036011, 0.04148700424555269, 0.3650747054636898, -0.32088546431295467, -0.2653982620423948, 0.10959289554821354, -0.3280198909639476, -0.16120965803094522, 0.1568114490077739, -0.09283203927432777,... |
710.2702 | Blob formation and acceleration in the solar wind: role of converging
flows and viscosity | The effect of viscosity and of converging flows on the formation of blobs in
the slow solar wind is analysed by means of resistive MHD simulations. The
regions above coronal streamers where blobs are formed (Sheeley et al., 1997)
are simulated using a model previously proposed by Einaudi et al. (1999). The
result of ... | astro-ph | the effect of viscosity and of converging flows on the formation of blobs in the slow solar wind is analysed by means of resistive mhd simulations the regions above coronal streamers where blobs are formed sheeley et al 1997 are simulated using a model previously proposed by einaudi et al 1999 the result of our investi... | [['the', 'effect', 'of', 'viscosity', 'and', 'of', 'converging', 'flows', 'on', 'the', 'formation', 'of', 'blobs', 'in', 'the', 'slow', 'solar', 'wind', 'is', 'analysed', 'by', 'means', 'of', 'resistive', 'mhd', 'simulations', 'the', 'regions', 'above', 'coronal', 'streamers', 'where', 'blobs', 'are', 'formed', 'sheele... | [-0.14761018981367374, 0.1880390705993852, -0.02077401523553842, 0.03996285621668338, -0.04514788929624735, -0.05287090850792624, 0.009166037872735714, 0.3229767528991844, -0.2347034214718922, -0.3390054140088929, 0.05578775208772198, -0.24169375382716188, -0.11876815131714416, 0.22524035335266712, -0.00999672669867003... |
710.2703 | Monte Carlo study of two-dimensional Bose-Hubbard model | One of the most promising applications of ultracold gases in optical lattices
is the possibility to use them as quantum emulators of more complex condensed
matter systems. We provide benchmark calculations, based on exact quantum Monte
Carlo simulations, for the emulator to be tested against. We report results for
th... | cond-mat.other cond-mat.stat-mech | one of the most promising applications of ultracold gases in optical lattices is the possibility to use them as quantum emulators of more complex condensed matter systems we provide benchmark calculations based on exact quantum monte carlo simulations for the emulator to be tested against we report results for the grou... | [['one', 'of', 'the', 'most', 'promising', 'applications', 'of', 'ultracold', 'gases', 'in', 'optical', 'lattices', 'is', 'the', 'possibility', 'to', 'use', 'them', 'as', 'quantum', 'emulators', 'of', 'more', 'complex', 'condensed', 'matter', 'systems', 'we', 'provide', 'benchmark', 'calculations', 'based', 'on', 'exac... | [-0.1251386811184746, 0.15054935498751307, -0.06605530681641758, 0.046515645798474295, 0.01370646725443745, -0.15355973966993897, 0.0921285501908847, 0.3525774858723906, -0.1969467464780183, -0.28958124208046976, 0.07227969322006982, -0.31050043334638266, -0.10311458731259227, 0.2025493831396509, 0.06460454591345988, 0... |
710.2704 | Low regularity solutions of two fifth-order KdV type equations | The Kawahara and modified Kawahara equations are fifth-order KdV type
equations and have been derived to model many physical phenomena such as
gravity-capillary waves and magneto-sound propagation in plasmas. This paper
establishes the local well-posedness of the initial-value problem for Kawahara
equation in $H^s({\... | math.AP math-ph math.MP | the kawahara and modified kawahara equations are fifthorder kdv type equations and have been derived to model many physical phenomena such as gravitycapillary waves and magnetosound propagation in plasmas this paper establishes the local wellposedness of the initialvalue problem for kawahara equation in hsmathbf r with... | [['the', 'kawahara', 'and', 'modified', 'kawahara', 'equations', 'are', 'fifthorder', 'kdv', 'type', 'equations', 'and', 'have', 'been', 'derived', 'to', 'model', 'many', 'physical', 'phenomena', 'such', 'as', 'gravitycapillary', 'waves', 'and', 'magnetosound', 'propagation', 'in', 'plasmas', 'this', 'paper', 'establis... | [-0.12821222822537126, 0.02675867371126702, -0.06921895689207379, 0.08806890259573678, -0.09505706866627041, -0.13193688482603, -0.06124675185923686, 0.2541332082611691, -0.32501899479581137, -0.23036796038912744, 0.15120316657343322, -0.2867583730114029, -0.1511176898913487, 0.21053128482140215, -0.029975366111383916,... |
710.2705 | Fingerprinting with Minimum Distance Decoding | This work adopts an information theoretic framework for the design of
collusion-resistant coding/decoding schemes for digital fingerprinting. More
specifically, the minimum distance decision rule is used to identify 1 out of t
pirates. Achievable rates, under this detection rule, are characterized in two
distinct sce... | cs.IT cs.CR math.IT | this work adopts an information theoretic framework for the design of collusionresistant codingdecoding schemes for digital fingerprinting more specifically the minimum distance decision rule is used to identify 1 out of t pirates achievable rates under this detection rule are characterized in two distinct scenarios fi... | [['this', 'work', 'adopts', 'an', 'information', 'theoretic', 'framework', 'for', 'the', 'design', 'of', 'collusionresistant', 'codingdecoding', 'schemes', 'for', 'digital', 'fingerprinting', 'more', 'specifically', 'the', 'minimum', 'distance', 'decision', 'rule', 'is', 'used', 'to', 'identify', '1', 'out', 'of', 't',... | [-0.1712097832500537, 0.039301877091958544, -0.07080367676869564, 0.08021062443754359, -0.011225862238968431, -0.23574097866096752, 0.12500579807476653, 0.3595771838371594, -0.2370118591550226, -0.26228876043803134, 0.12038090489777137, -0.2559635200880085, -0.14373795377558074, 0.20479772855774334, -0.1065369831607953... |
710.2706 | Kawamata-Viehweg Vanishing on Rational Surfaces in Positive
Characteristic | We prove that the Kawamata-Viehweg vanishing theorem holds on rational
surfaces in positive characteristic by means of the lifting property to W_2(k)
of certain log pairs on smooth rational surfaces. As a corollary, the
Kawamata-Viehweg vanishing theorem holds on log del Pezzo surfaces in positive
characteristic.
| math.AG | we prove that the kawamataviehweg vanishing theorem holds on rational surfaces in positive characteristic by means of the lifting property to w_2k of certain log pairs on smooth rational surfaces as a corollary the kawamataviehweg vanishing theorem holds on log del pezzo surfaces in positive characteristic | [['we', 'prove', 'that', 'the', 'kawamataviehweg', 'vanishing', 'theorem', 'holds', 'on', 'rational', 'surfaces', 'in', 'positive', 'characteristic', 'by', 'means', 'of', 'the', 'lifting', 'property', 'to', 'w_2k', 'of', 'certain', 'log', 'pairs', 'on', 'smooth', 'rational', 'surfaces', 'as', 'a', 'corollary', 'the', '... | [-0.27588260232321615, 0.016769764588072732, -0.1259255339593991, 0.15487383686653947, -0.0306781859582533, -0.23846500313273913, 0.03589323648939962, 0.23787817974453387, -0.2939260472826984, -0.206209742585602, 0.03129675308667609, -0.25453772800772084, -0.13973850497732992, 0.29196355103150656, -0.21216622827088702,... |
710.2707 | The Polyakov Loop and the Eigenvalues of the Dirac Operator | Aiming at the link between confinement and chiral symmetry the Polyakov loop
represented as a spectral sum of eigenvalues of the Dirac operator was subject
of recent studies. We analyze the volume dependence as well as the continuum
behavior of this quantity for quenched QCD using staggered fermions.
Furthermore, we ... | hep-lat | aiming at the link between confinement and chiral symmetry the polyakov loop represented as a spectral sum of eigenvalues of the dirac operator was subject of recent studies we analyze the volume dependence as well as the continuum behavior of this quantity for quenched qcd using staggered fermions furthermore we prese... | [['aiming', 'at', 'the', 'link', 'between', 'confinement', 'and', 'chiral', 'symmetry', 'the', 'polyakov', 'loop', 'represented', 'as', 'a', 'spectral', 'sum', 'of', 'eigenvalues', 'of', 'the', 'dirac', 'operator', 'was', 'subject', 'of', 'recent', 'studies', 'we', 'analyze', 'the', 'volume', 'dependence', 'as', 'well'... | [-0.13710271861470705, 0.18158042242118558, -0.10173194277116895, 0.05087651527511688, -0.021799871448560486, -0.051326698625676466, 0.08287456137311112, 0.3826316838551845, -0.16829049263781468, -0.27011120977944564, 0.08100345549506269, -0.2881369104143232, -0.17060167107930674, 0.06601650514806222, 0.034247385944971... |
710.2708 | Hodge-theoretic aspects of the Decomposition Theorem | Given a projective morphism of compact, complex, algebraic varieties and a
relatively ample line bundle on the domain we prove that a suitable choice,
dictated by the line bundle, of the decomposition isomorphism of the
Decomposition Theorem of Beilinson, Bernstein, Deligne and Gabber, yields
isomorphisms of pure Hod... | math.AG | given a projective morphism of compact complex algebraic varieties and a relatively ample line bundle on the domain we prove that a suitable choice dictated by the line bundle of the decomposition isomorphism of the decomposition theorem of beilinson bernstein deligne and gabber yields isomorphisms of pure hodge struct... | [['given', 'a', 'projective', 'morphism', 'of', 'compact', 'complex', 'algebraic', 'varieties', 'and', 'a', 'relatively', 'ample', 'line', 'bundle', 'on', 'the', 'domain', 'we', 'prove', 'that', 'a', 'suitable', 'choice', 'dictated', 'by', 'the', 'line', 'bundle', 'of', 'the', 'decomposition', 'isomorphism', 'of', 'the... | [-0.2468555912746524, -0.032375421336231135, -0.14854737626349865, 0.08560486015267088, -0.156030463889086, -0.12837250850861892, 0.01713924111390952, 0.3019688129273466, -0.39703846140764654, -0.180188214823526, 0.12061045381172637, -0.16320631320316656, -0.14778897781313086, 0.1622974412360539, -0.23242935299640521, ... |
710.2709 | Dynamical black holes with symmetry in Einstein-Gauss-Bonnet gravity | We explore various aspects of dynamical black holes defined by a future outer
trapping horizon in $n(\ge 5)$-dimensional Einstein-Gauss-Bonnet gravity. In
the present paper, we assume that the spacetime has symmetries corresponding to
the isometries of an $(n-2)$-dimensional maximally symmetric space and the
Gauss-Bo... | gr-qc hep-th | we explore various aspects of dynamical black holes defined by a future outer trapping horizon in nge 5dimensional einsteingaussbonnet gravity in the present paper we assume that the spacetime has symmetries corresponding to the isometries of an n2dimensional maximally symmetric space and the gaussbonnet coupling const... | [['we', 'explore', 'various', 'aspects', 'of', 'dynamical', 'black', 'holes', 'defined', 'by', 'a', 'future', 'outer', 'trapping', 'horizon', 'in', 'nge', '5dimensional', 'einsteingaussbonnet', 'gravity', 'in', 'the', 'present', 'paper', 'we', 'assume', 'that', 'the', 'spacetime', 'has', 'symmetries', 'corresponding', ... | [-0.16410627742203873, 0.1143561453780311, -0.12493196281491581, 0.09089607911918199, -0.09761062034669173, -0.132252906101951, -0.022713443294938917, 0.32350947079248726, -0.2229684830179927, -0.23814501927582302, 0.09883738527100326, -0.28130660917741634, -0.09474005187377145, 0.16434831837676653, -0.0841111677035576... |
710.271 | Fluctuation-dissipation theorem for thermo-refractive noise | We introduce a simple prescription for calculating the spectra of thermal
fluctuations of temperature-dependent quantities of the form $\hat{\delta
T}(t)=\int d^3\vec{r} \delta T(\vec{r},t) q(\vec{r})$. Here $T(\vec{r}, t)$ is
the local temperature at location $\vec{r}$ and time $t$, and $q(\vec{r})$ is
an arbitrary ... | cond-mat.stat-mech astro-ph gr-qc | we introduce a simple prescription for calculating the spectra of thermal fluctuations of temperaturedependent quantities of the form hatdelta ttint d3vecr delta tvecrt qvecr here tvecr t is the local temperature at location vecr and time t and qvecr is an arbitrary function as an example of a possible application we c... | [['we', 'introduce', 'a', 'simple', 'prescription', 'for', 'calculating', 'the', 'spectra', 'of', 'thermal', 'fluctuations', 'of', 'temperaturedependent', 'quantities', 'of', 'the', 'form', 'hatdelta', 'ttint', 'd3vecr', 'delta', 'tvecrt', 'qvecr', 'here', 'tvecr', 't', 'is', 'the', 'local', 'temperature', 'at', 'locat... | [-0.1217746314611862, 0.11156374810187905, -0.06694041957272236, 0.030748966191991318, -0.014170377695280099, -0.08647355302861057, 0.040389177559865354, 0.34074890302474964, -0.2016410252088969, -0.29874240367951777, 0.06746076665501849, -0.2995580752985072, -0.12302387533613394, 0.21227855757406922, -0.02864463400268... |
710.2711 | High photo-excited carrier multiplication by charged InAs dots in
AlAs/GaAs/AlAs resonant tunneling diode | We present an approach for the highly sensitive photon detection based on the
quantum dots (QDs) operating at temperature of 77K. The detection structure is
based on an AlAs/GaAs/AlAs double barrier resonant tunneling diode combined
with a layer of self-assembled InAs QDs (QD-RTD). A photon rate of 115 photons
per se... | quant-ph | we present an approach for the highly sensitive photon detection based on the quantum dots qds operating at temperature of 77k the detection structure is based on an alasgaasalas double barrier resonant tunneling diode combined with a layer of selfassembled inas qds qdrtd a photon rate of 115 photons per second had ind... | [['we', 'present', 'an', 'approach', 'for', 'the', 'highly', 'sensitive', 'photon', 'detection', 'based', 'on', 'the', 'quantum', 'dots', 'qds', 'operating', 'at', 'temperature', 'of', '77k', 'the', 'detection', 'structure', 'is', 'based', 'on', 'an', 'alasgaasalas', 'double', 'barrier', 'resonant', 'tunneling', 'diode... | [-0.16837842032751615, 0.1858801759960924, -0.005531570090747931, -0.029973423201590778, 0.04302243957953418, -0.18720952845452463, 0.10339487768600092, 0.4158424818669172, -0.2521049318835139, -0.34075920632218615, -0.031342445118078856, -0.29478016214630126, -0.08526921094778706, 0.2436311240581905, 0.006109625024392... |
710.2712 | The structures of standard (g,K)-modules of SL(3,R) | We describe explicitely the structures of standard $(g,K)$-modules of
$SL(3,R)$.
| math.RT math.NT | we describe explicitely the structures of standard gkmodules of sl3r | [['we', 'describe', 'explicitely', 'the', 'structures', 'of', 'standard', 'gkmodules', 'of', 'sl3r']] | [-0.1381894551217556, 0.0692022212781012, -0.11217985954135656, 0.1427380360662937, -0.06651121098548174, -0.015386165678501129, -0.05653336681425571, 0.3479719690978527, -0.33371311640366913, -0.16350034885108472, 0.04732484663836658, -0.17099234983325004, -0.22260951101779938, 0.12078225314617157, -0.1117032868787646... |
710.2713 | Leptonic CP Violation Induced by Approximately mu-tau Symmetric Seesaw
Mechanism | Assuming a minimal seesaw model with two heavy neutrinos (N), we examine
effects of leptonic CP violation induced by approximate mu-tau symmetric
interactions. As long as N is subject to the mu-tau symmetry, we can choose CP
phases of Dirac mass terms without loss of generality in such a way that these
phases arise f... | hep-ph | assuming a minimal seesaw model with two heavy neutrinos n we examine effects of leptonic cp violation induced by approximate mutau symmetric interactions as long as n is subject to the mutau symmetry we can choose cp phases of dirac mass terms without loss of generality in such a way that these phases arise from mutau... | [['assuming', 'a', 'minimal', 'seesaw', 'model', 'with', 'two', 'heavy', 'neutrinos', 'n', 'we', 'examine', 'effects', 'of', 'leptonic', 'cp', 'violation', 'induced', 'by', 'approximate', 'mutau', 'symmetric', 'interactions', 'as', 'long', 'as', 'n', 'is', 'subject', 'to', 'the', 'mutau', 'symmetry', 'we', 'can', 'choo... | [-0.16413942018698435, 0.3218705619268197, 0.024541707571491617, 0.14477537395396212, -0.09897720660471047, -0.22745415096142096, 0.07378261207365237, 0.3436906736387755, -0.2537017060221842, -0.3074255992930072, 0.06032245100565584, -0.28330448070588926, -0.07311438099259249, 0.04740314704395132, 0.05305083255370846, ... |
710.2714 | On the Brink of Major Discoveries in Weak Charm Decays -- a Bismarckian
Chance to Make History | The recently obtained strong evidence for $D^0 - \bar D^0$ oscillations from
the $B$ factories provides an important benchmark in our search for New Physics
in charm transitions. While the theoretical verdict on the observed values of
$x_D$ and $y_D$ is ambiguous -- they could be fully generated by SM dynamics,
yet c... | hep-ph | the recently obtained strong evidence for d0 bar d0 oscillations from the b factories provides an important benchmark in our search for new physics in charm transitions while the theoretical verdict on the observed values of x_d and y_d is ambiguous they could be fully generated by sm dynamics yet could contain also a ... | [['the', 'recently', 'obtained', 'strong', 'evidence', 'for', 'd0', 'bar', 'd0', 'oscillations', 'from', 'the', 'b', 'factories', 'provides', 'an', 'important', 'benchmark', 'in', 'our', 'search', 'for', 'new', 'physics', 'in', 'charm', 'transitions', 'while', 'the', 'theoretical', 'verdict', 'on', 'the', 'observed', '... | [-0.051858969218027524, 0.24246372336221944, -0.07994680302167531, 0.14489366895874703, -0.08584247779862214, -0.1776421357807453, 0.08288884339278303, 0.2523483607958081, -0.27235529601814285, -0.2729022013804605, 0.01953611944574282, -0.31298070035434217, -0.05711048287189295, 0.19422060102775132, 0.03592890149022462... |
710.2715 | Off-shell dimensional reduction of 5D orbifold supergravity | We present a systematic way for deriving a four-dimensional (4D) effective
action of the five-dimensional (5D) orbifold supergravity respecting the N=1
{\it off-shell} structure. As an illustrating example, we derive a 4D effective
theory of the 5D gauged supergravity with a universal hypermultiplet and {\it
generic}... | hep-th hep-ph | we present a systematic way for deriving a fourdimensional 4d effective action of the fivedimensional 5d orbifold supergravity respecting the n1 it offshell structure as an illustrating example we derive a 4d effective theory of the 5d gauged supergravity with a universal hypermultiplet and it generic gaugings which in... | [['we', 'present', 'a', 'systematic', 'way', 'for', 'deriving', 'a', 'fourdimensional', '4d', 'effective', 'action', 'of', 'the', 'fivedimensional', '5d', 'orbifold', 'supergravity', 'respecting', 'the', 'n1', 'it', 'offshell', 'structure', 'as', 'an', 'illustrating', 'example', 'we', 'derive', 'a', '4d', 'effective', ... | [-0.13051849117354405, 0.12946266061457704, 0.0017554086199114945, 0.13903931165325709, -0.11112299549346392, -0.1766907707576386, -0.004371092558192851, 0.2658144814724272, -0.1287202594500162, -0.2826679474991662, 0.059886416036699135, -0.24424930254727686, -0.21812670536085285, 0.05059448019230992, -0.08097975161879... |
710.2716 | Cost and Effects of Pinning Control for Network Synchronization | In this paper, the problem of pinning control for synchronization of complex
dynamical networks is discussed. A cost function of the controlled network is
defined by the feedback gain and the coupling strength of the network. An
interesting result is that lower cost is achieved by the control scheme of
pinning nodes ... | cs.NI | in this paper the problem of pinning control for synchronization of complex dynamical networks is discussed a cost function of the controlled network is defined by the feedback gain and the coupling strength of the network an interesting result is that lower cost is achieved by the control scheme of pinning nodes with ... | [['in', 'this', 'paper', 'the', 'problem', 'of', 'pinning', 'control', 'for', 'synchronization', 'of', 'complex', 'dynamical', 'networks', 'is', 'discussed', 'a', 'cost', 'function', 'of', 'the', 'controlled', 'network', 'is', 'defined', 'by', 'the', 'feedback', 'gain', 'and', 'the', 'coupling', 'strength', 'of', 'the'... | [-0.2042798320453198, 0.07303468520060166, 0.014306143451323534, 0.04564239360649693, -0.034984977202529605, -0.16376853139917466, 0.045034356010295054, 0.3844653404951888, -0.26154429175237076, -0.30152171511361575, 0.09354377338573575, -0.21800819090369375, -0.23655964348940772, 0.21723670674676193, -0.06636103504941... |
710.2717 | Probing Nonequilibrium Fluctuations through Linear Response | Linear response analysis in the nonequilibrium steady state (Gaussian regime)
provides two independent fluctuation-response relations. One, in the form of
the symmetric matrix, manifests the departure from the equilibrium formula
through the quantity so-called {\it irreversible circulation}. The other, in
the anti-sy... | cond-mat.stat-mech cond-mat.soft | linear response analysis in the nonequilibrium steady state gaussian regime provides two independent fluctuationresponse relations one in the form of the symmetric matrix manifests the departure from the equilibrium formula through the quantity socalled it irreversible circulation the other in the antisymmetric form co... | [['linear', 'response', 'analysis', 'in', 'the', 'nonequilibrium', 'steady', 'state', 'gaussian', 'regime', 'provides', 'two', 'independent', 'fluctuationresponse', 'relations', 'one', 'in', 'the', 'form', 'of', 'the', 'symmetric', 'matrix', 'manifests', 'the', 'departure', 'from', 'the', 'equilibrium', 'formula', 'thr... | [-0.13237874086813203, 0.14463442022513065, -0.1915336996716048, 0.07664094479322167, -0.015477901218192917, -0.1027992914297751, 0.026581615768373014, 0.2665794295125774, -0.29786021797252554, -0.22387613935030198, 0.059878908521828374, -0.3300816705716508, -0.15726272430537003, 0.14445038001452173, 0.0656896306012640... |
710.2718 | Stochastic resonance in a single electron turnstile | In this paper, we report stochastic resonance (SR) in a single electron
turnstile. It has been known that SR emerges by the cooperation of a weak
periodic signal and noise in a bistable system. A periodic signal produces
switching between two stable states by lowering the potential barrier. Even if
the amplitude of t... | quant-ph | in this paper we report stochastic resonance sr in a single electron turnstile it has been known that sr emerges by the cooperation of a weak periodic signal and noise in a bistable system a periodic signal produces switching between two stable states by lowering the potential barrier even if the amplitude of the signa... | [['in', 'this', 'paper', 'we', 'report', 'stochastic', 'resonance', 'sr', 'in', 'a', 'single', 'electron', 'turnstile', 'it', 'has', 'been', 'known', 'that', 'sr', 'emerges', 'by', 'the', 'cooperation', 'of', 'a', 'weak', 'periodic', 'signal', 'and', 'noise', 'in', 'a', 'bistable', 'system', 'a', 'periodic', 'signal', ... | [-0.1770971324589943, 0.1573133255351166, -0.05706381803693276, 0.03965320513898533, -0.011657253839075565, -0.1760932228849335, 0.08576867182929279, 0.3707670951868788, -0.29045375158131437, -0.291694597521482, 0.07381887922004442, -0.2313818737182399, -0.16450571429646824, 0.1911003123755685, -0.06802841423827052, 0.... |
710.2719 | Branes on Poisson varieties | We first extend the notion of connection in the context of Courant algebroids
to obtain a new characterization of generalized Kaehler geometry. We then
establish a new notion of isomorphism between holomorphic Poisson manifolds,
which is non-holomorphic in nature. Finally we show an equivalence between
certain config... | math.DG hep-th math.SG | we first extend the notion of connection in the context of courant algebroids to obtain a new characterization of generalized kaehler geometry we then establish a new notion of isomorphism between holomorphic poisson manifolds which is nonholomorphic in nature finally we show an equivalence between certain configuratio... | [['we', 'first', 'extend', 'the', 'notion', 'of', 'connection', 'in', 'the', 'context', 'of', 'courant', 'algebroids', 'to', 'obtain', 'a', 'new', 'characterization', 'of', 'generalized', 'kaehler', 'geometry', 'we', 'then', 'establish', 'a', 'new', 'notion', 'of', 'isomorphism', 'between', 'holomorphic', 'poisson', 'm... | [-0.19949979267697385, 0.004778431692102458, -0.0744027841236799, 0.15226752098966786, -0.204204589009602, -0.1619139129117607, -0.01280911819652674, 0.3573406155201349, -0.3139150690762921, -0.2254527123803471, 0.04933670874774218, -0.2056729203743979, -0.26937104396997613, 0.16972998957684698, -0.19275320546473673, -... |
710.272 | Schubert Polynomials for the affine Grassmannian of the symplectic group | We study the Schubert calculus of the affine Grassmannian Gr of the
symplectic group. The integral homology and cohomology rings of Gr are
identified with dual Hopf algebras of symmetric functions, defined in terms of
Schur's P and Q-functions. An explicit combinatorial description is obtained
for the Schubert basis ... | math.CO math.AG | we study the schubert calculus of the affine grassmannian gr of the symplectic group the integral homology and cohomology rings of gr are identified with dual hopf algebras of symmetric functions defined in terms of schurs p and qfunctions an explicit combinatorial description is obtained for the schubert basis of the ... | [['we', 'study', 'the', 'schubert', 'calculus', 'of', 'the', 'affine', 'grassmannian', 'gr', 'of', 'the', 'symplectic', 'group', 'the', 'integral', 'homology', 'and', 'cohomology', 'rings', 'of', 'gr', 'are', 'identified', 'with', 'dual', 'hopf', 'algebras', 'of', 'symmetric', 'functions', 'defined', 'in', 'terms', 'of... | [-0.19415981538424437, -0.013507672635486497, -0.10543299812442539, 0.07635681793908589, -0.12834245919789697, -0.15914829029299488, -0.030838590729135005, 0.2894788713363761, -0.3668002587669021, -0.1661791943267665, 0.08892398618296614, -0.1460608803450172, -0.18597574211889878, 0.15251209036531774, -0.17780729957898... |
710.2721 | Large nonlinear absorption and refraction coefficients of carbon
nanotubes estimated from femtosecond Z-scan measurements | Nonlinear transmission of 80 and 140 femtosecond pulsed light with $0.79 \mu
m$ wavelength through single walled carbon nanotubes suspended in water
containing sodium dodecyl sulphate is studied. Pulse-width independent
saturation absorption and negative cubic nonlinearity are observed,
respectively, in open and clos... | cond-mat.mtrl-sci | nonlinear transmission of 80 and 140 femtosecond pulsed light with 079 mu m wavelength through single walled carbon nanotubes suspended in water containing sodium dodecyl sulphate is studied pulsewidth independent saturation absorption and negative cubic nonlinearity are observed respectively in open and closed apertur... | [['nonlinear', 'transmission', 'of', '80', 'and', '140', 'femtosecond', 'pulsed', 'light', 'with', '079', 'mu', 'm', 'wavelength', 'through', 'single', 'walled', 'carbon', 'nanotubes', 'suspended', 'in', 'water', 'containing', 'sodium', 'dodecyl', 'sulphate', 'is', 'studied', 'pulsewidth', 'independent', 'saturation', ... | [-0.11147214068123737, 0.15339644507576639, 0.05019792545443544, -0.027029358505760916, -0.009422396467879223, -0.23493636884869865, 0.0681044638921053, 0.475365627461519, -0.19826415116683796, -0.33522836081922436, 0.0557173369347882, -0.3643639338537095, -0.028952591761481017, 0.21277747553092644, 0.02213280550084817... |
710.2722 | The 2006 Radio Outburst of a Microquasar Cyg X-3: Observation and Data | We present the results of the multi-frequency observations of radio outburst
of the microquasar Cyg X-3 in February and March 2006 with the Nobeyama 45-m
telescope, the Nobeyama Millimeter Array, and the Yamaguchi 32-m telescope.
Since the prediction of a flare by RATAN-600, the source has been monitored
from Jan 27 ... | astro-ph | we present the results of the multifrequency observations of radio outburst of the microquasar cyg x3 in february and march 2006 with the nobeyama 45m telescope the nobeyama millimeter array and the yamaguchi 32m telescope since the prediction of a flare by ratan600 the source has been monitored from jan 27 ut with the... | [['we', 'present', 'the', 'results', 'of', 'the', 'multifrequency', 'observations', 'of', 'radio', 'outburst', 'of', 'the', 'microquasar', 'cyg', 'x3', 'in', 'february', 'and', 'march', '2006', 'with', 'the', 'nobeyama', '45m', 'telescope', 'the', 'nobeyama', 'millimeter', 'array', 'and', 'the', 'yamaguchi', '32m', 'te... | [-0.12068193248303244, 0.13708931401609178, -0.040494007510923836, 0.015737186037384724, -0.05649019779532023, -0.09623736146480173, 0.056096765221500734, 0.44359431127320575, -0.13622703344441084, -0.3960407395158351, 0.17473989784418834, -0.2904305996800884, -0.06518587630546693, 0.18496667757431198, -0.0120971062039... |
710.2723 | Boundary conditions for Dirac fermions on a terminated honeycomb lattice | We derive the boundary condition for the Dirac equation corresponding to a
tight-binding model on a two-dimensional honeycomb lattice terminated along an
arbitary direction. Zigzag boundary conditions result generically once the
boundary is not parallel to the bonds. Since a honeycomb strip with zigzag
edges is gaple... | cond-mat.mes-hall | we derive the boundary condition for the dirac equation corresponding to a tightbinding model on a twodimensional honeycomb lattice terminated along an arbitary direction zigzag boundary conditions result generically once the boundary is not parallel to the bonds since a honeycomb strip with zigzag edges is gapless thi... | [['we', 'derive', 'the', 'boundary', 'condition', 'for', 'the', 'dirac', 'equation', 'corresponding', 'to', 'a', 'tightbinding', 'model', 'on', 'a', 'twodimensional', 'honeycomb', 'lattice', 'terminated', 'along', 'an', 'arbitary', 'direction', 'zigzag', 'boundary', 'conditions', 'result', 'generically', 'once', 'the',... | [-0.2375254942458277, 0.18088511391547663, -0.05166453994379556, -0.005118301826190542, -0.06988466436414756, -0.21953477917916395, 0.07695042130283335, 0.4150955748151649, -0.27286189420472, -0.2060067256650895, 0.07444428870635307, -0.26666840694244365, -0.12798652739825944, 0.07022233957170763, 0.008831536043281397,... |
710.2724 | General Solution of the Quantum Damped Harmonic Oscillator | In this paper the general solution of the quantum damped harmonic oscillator
is given.
| quant-ph math-ph math.MP | in this paper the general solution of the quantum damped harmonic oscillator is given | [['in', 'this', 'paper', 'the', 'general', 'solution', 'of', 'the', 'quantum', 'damped', 'harmonic', 'oscillator', 'is', 'given']] | [-0.14546734453844173, 0.14223784620740584, 0.012593648263386317, -0.0471389251095908, -0.03656026601259198, -0.18457395769655704, -0.04508584645476991, 0.2697767343904291, -0.24581131871257508, -0.13232560203011548, 0.03479994583176449, -0.2958540243229696, -0.2514869709100042, 0.2211998738348484, -0.09326386079192162... |
710.2725 | A moduli scheme of embedded curve singularities | The main purpose of this paper is to prove the existence of the moduli space
parameterizing the embedded curve singularities of $(k^N,0)$ with an admissible
Hilbert polynomial and to study its basic properties.
| math.AG math.AC | the main purpose of this paper is to prove the existence of the moduli space parameterizing the embedded curve singularities of kn0 with an admissible hilbert polynomial and to study its basic properties | [['the', 'main', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'prove', 'the', 'existence', 'of', 'the', 'moduli', 'space', 'parameterizing', 'the', 'embedded', 'curve', 'singularities', 'of', 'kn0', 'with', 'an', 'admissible', 'hilbert', 'polynomial', 'and', 'to', 'study', 'its', 'basic', 'properties']] | [-0.17997889395337552, 0.031338292032614845, -0.1412881498108618, 0.033857544214697555, -0.09653909527696669, -0.025943168831872754, -0.055583636476512766, 0.2819065325311385, -0.37200187146663666, -0.18147544730163645, 0.12490707274992019, -0.1913795324799139, -0.1705365613452159, 0.1840739722683793, -0.14207046566298... |
710.2726 | Log Structures on Generalized Semi-Stable Varieties | This is my PhD Thesis, part of it has published in Acta Mathematica Sinica.
In this paper, a class of morphisms which have a kind of singularity weaker
than normal crossing is considered. We construct the obstruction such that the
so-called semi-stable log structures exists if and only if the obstruction
vanishes. In... | math.AG | this is my phd thesis part of it has published in acta mathematica sinica in this paper a class of morphisms which have a kind of singularity weaker than normal crossing is considered we construct the obstruction such that the socalled semistable log structures exists if and only if the obstruction vanishes in the case... | [['this', 'is', 'my', 'phd', 'thesis', 'part', 'of', 'it', 'has', 'published', 'in', 'acta', 'mathematica', 'sinica', 'in', 'this', 'paper', 'a', 'class', 'of', 'morphisms', 'which', 'have', 'a', 'kind', 'of', 'singularity', 'weaker', 'than', 'normal', 'crossing', 'is', 'considered', 'we', 'construct', 'the', 'obstruct... | [-0.16560162333022246, 0.039235193111088085, -0.126233602799047, 0.07895323886782274, -0.1282774338006288, -0.13283910131317445, -0.006774076741006782, 0.31349437555362436, -0.30135494737147256, -0.23998413377323713, 0.07457784214057028, -0.2618604523996855, -0.1896258378080253, 0.14266088129631405, -0.1278458550283364... |
710.2727 | Effect of contact induced states on minimum conductivity in graphene | The objective of this paper is to point out that contact induced states can
help explain the structure dependence of the minimum conductivity observed
experimentally even if the samples were purely ballistic. Contact induced
states are similar to the well-known metal induced gap states (MIGS) in
metal-semiconductor S... | cond-mat.mes-hall | the objective of this paper is to point out that contact induced states can help explain the structure dependence of the minimum conductivity observed experimentally even if the samples were purely ballistic contact induced states are similar to the wellknown metal induced gap states migs in metalsemiconductor schottky... | [['the', 'objective', 'of', 'this', 'paper', 'is', 'to', 'point', 'out', 'that', 'contact', 'induced', 'states', 'can', 'help', 'explain', 'the', 'structure', 'dependence', 'of', 'the', 'minimum', 'conductivity', 'observed', 'experimentally', 'even', 'if', 'the', 'samples', 'were', 'purely', 'ballistic', 'contact', 'in... | [-0.14444940780653182, 0.19980320141970362, -0.06085274665004756, 0.051867217225705954, -0.04177750958151807, -0.15321265125217345, 0.07642292891168889, 0.4026541652890837, -0.2884506532321712, -0.3149513815083271, 0.013213775112409388, -0.3312655690638624, -0.13457148524515122, 0.20200870194907725, 0.00735980271190933... |
710.2728 | Primes in Tuples II | We prove that there are infinitely often pairs of primes much closer than the
average spacing between primes - almost within the square root of the average
spacing. We actually prove a more general result concerning the set of values
taken on by the differences between primes.
| math.NT | we prove that there are infinitely often pairs of primes much closer than the average spacing between primes almost within the square root of the average spacing we actually prove a more general result concerning the set of values taken on by the differences between primes | [['we', 'prove', 'that', 'there', 'are', 'infinitely', 'often', 'pairs', 'of', 'primes', 'much', 'closer', 'than', 'the', 'average', 'spacing', 'between', 'primes', 'almost', 'within', 'the', 'square', 'root', 'of', 'the', 'average', 'spacing', 'we', 'actually', 'prove', 'a', 'more', 'general', 'result', 'concerning', ... | [-0.18087968633904972, 0.12929494237608236, -0.10782409499844779, 0.1496541197411716, 0.05536550222693578, -0.07752425465530352, 0.08113462425282468, 0.3533528008214805, -0.23541475913446883, -0.3016178488083508, 0.020788862299093085, -0.32808517522947944, -0.08291046272295163, 0.23659136429752992, -0.06391813080130226... |
710.2729 | Light localization signatures in backscattering from periodic disordered
media | The backscattering line shape is analytically predicted for thick disordered
medium films where, remarkably, the medium configuration is periodic along the
direction perpendicular to the incident light. A blunt triangular peak is found
to emerge on the sharp top. The phenomenon roots in the coexistence of quasi-1D
lo... | cond-mat.dis-nn cond-mat.mes-hall | the backscattering line shape is analytically predicted for thick disordered medium films where remarkably the medium configuration is periodic along the direction perpendicular to the incident light a blunt triangular peak is found to emerge on the sharp top the phenomenon roots in the coexistence of quasi1d localizat... | [['the', 'backscattering', 'line', 'shape', 'is', 'analytically', 'predicted', 'for', 'thick', 'disordered', 'medium', 'films', 'where', 'remarkably', 'the', 'medium', 'configuration', 'is', 'periodic', 'along', 'the', 'direction', 'perpendicular', 'to', 'the', 'incident', 'light', 'a', 'blunt', 'triangular', 'peak', '... | [-0.18417939980281517, 0.1875944298394293, -0.04611807000429298, 0.03647668265442077, -0.045830512553668365, -0.16937113609702253, 0.003991612009345912, 0.4379106733518151, -0.2775729532765511, -0.2153042410321247, 0.025655881221889734, -0.31780776184258197, -0.10385182037806281, 0.15973611253922662, 0.0468503816877133... |
710.273 | Lattice simulation of 2+1 flavors of overlap light quarks | We report on the status of the dynamical overlap QCD simulation project by
the JLQCD collaboration. After completing two-flavor QCD simulation on a
16^3x32 lattice at lattice spacing a 0.12 fm, we started a series of runs with
2+1 flavors. In this report, we describe an outline of our algorithms,
parameter choices, a... | hep-lat | we report on the status of the dynamical overlap qcd simulation project by the jlqcd collaboration after completing twoflavor qcd simulation on a 163x32 lattice at lattice spacing a 012 fm we started a series of runs with 21 flavors in this report we describe an outline of our algorithms parameter choices and some earl... | [['we', 'report', 'on', 'the', 'status', 'of', 'the', 'dynamical', 'overlap', 'qcd', 'simulation', 'project', 'by', 'the', 'jlqcd', 'collaboration', 'after', 'completing', 'twoflavor', 'qcd', 'simulation', 'on', 'a', '163x32', 'lattice', 'at', 'lattice', 'spacing', 'a', '012', 'fm', 'we', 'started', 'a', 'series', 'of'... | [-0.1343486230180133, 0.20468861657923298, -0.1232165103629086, -0.022191861376995803, -0.014099358675593976, -0.0004010546563222306, 0.1258543082349206, 0.3840382145863259, -0.11648049735231325, -0.27647463759421953, 0.14263463755014527, -0.2824153327383101, -0.10477048396387545, 0.11166421236703172, 0.031614629653631... |
710.2731 | Group Analysis of Variable Coefficient Diffusion-Convection Equations.
I. Enhanced Group Classification | We discuss the classical statement of group classification problem and some
its extensions in the general case. After that, we carry out the complete
extended group classification for a class of (1+1)-dimensional nonlinear
diffusion--convection equations with coefficients depending on the space
variable. At first, we... | math-ph math.AP math.MP | we discuss the classical statement of group classification problem and some its extensions in the general case after that we carry out the complete extended group classification for a class of 11dimensional nonlinear diffusionconvection equations with coefficients depending on the space variable at first we construct t... | [['we', 'discuss', 'the', 'classical', 'statement', 'of', 'group', 'classification', 'problem', 'and', 'some', 'its', 'extensions', 'in', 'the', 'general', 'case', 'after', 'that', 'we', 'carry', 'out', 'the', 'complete', 'extended', 'group', 'classification', 'for', 'a', 'class', 'of', '11dimensional', 'nonlinear', 'd... | [-0.12545181099376101, 0.061032722689461624, -0.08629145811875763, 0.04829498448767097, -0.10491544182798794, -0.1241050926100488, 0.03131832455151847, 0.36119757127788926, -0.2684418040778738, -0.27365794468340054, 0.11558317423316644, -0.24410395854335679, -0.135876449062584, 0.16958050050956458, -0.03858324154882001... |
710.2732 | Probabilistic communication complexity over the reals | Deterministic and probabilistic communication protocols are introduced in
which parties can exchange the values of polynomials (rather than bits in the
usual setting). It is established a sharp lower bound $2n$ on the communication
complexity of recognizing the $2n$-dimensional orthant, on the other hand the
probabil... | cs.CC | deterministic and probabilistic communication protocols are introduced in which parties can exchange the values of polynomials rather than bits in the usual setting it is established a sharp lower bound 2n on the communication complexity of recognizing the 2ndimensional orthant on the other hand the probabilistic commu... | [['deterministic', 'and', 'probabilistic', 'communication', 'protocols', 'are', 'introduced', 'in', 'which', 'parties', 'can', 'exchange', 'the', 'values', 'of', 'polynomials', 'rather', 'than', 'bits', 'in', 'the', 'usual', 'setting', 'it', 'is', 'established', 'a', 'sharp', 'lower', 'bound', '2n', 'on', 'the', 'commu... | [-0.19333747703785775, 0.10552922988426872, -0.035418806228941925, 0.0924629032372953, -0.05758231096357728, -0.22397929886938073, 0.1187285562142885, 0.2801247095533957, -0.262306006567087, -0.29333275579847395, 0.1087831498941038, -0.24608132540015504, -0.1255367809596161, 0.23535740829781085, -0.14083066358580254, 0... |
710.2733 | Breakdown of Coherence ? | In a recent paper, Albrecht Kyrieleis, Jeff Forshaw and I discovered a new
tower of super-leading logarithms in gaps between jets cross sections. After
discussions with the referee of our paper and further investigation, we have
come to view this as a breakdown of naive coherence for initial state
radiation. In this ... | hep-ph | in a recent paper albrecht kyrieleis jeff forshaw and i discovered a new tower of superleading logarithms in gaps between jets cross sections after discussions with the referee of our paper and further investigation we have come to view this as a breakdown of naive coherence for initial state radiation in this talk i i... | [['in', 'a', 'recent', 'paper', 'albrecht', 'kyrieleis', 'jeff', 'forshaw', 'and', 'i', 'discovered', 'a', 'new', 'tower', 'of', 'superleading', 'logarithms', 'in', 'gaps', 'between', 'jets', 'cross', 'sections', 'after', 'discussions', 'with', 'the', 'referee', 'of', 'our', 'paper', 'and', 'further', 'investigation', ... | [-0.10266454202492777, 0.10382440124008366, -0.15164507857030807, 0.08297957617084167, -0.0267486124409034, -0.06735526579980027, 0.08167097463121857, 0.34416960292112303, -0.2255943836096455, -0.30334642752046315, 0.04286357630831737, -0.2827419925700216, -0.15602986405343366, 0.14116139860604615, -0.07368646274485133... |
710.2734 | Quark Masses in Supersymmetric SU(3)color x SU(3)W x U(1)X Model with
Discrete T' flavor symmetry | We propose a supersymmetric model of quark flavor symmetry based on
SU(3)colorxSU(3)WxU(1)X x T' where T' (binary tetrahedral group) is a discrete
flavor symmetry group. The third (heavy) generation of quarks are assigned to
singlet representation of T' while light quark generations are treated
differently and assign... | hep-ph | we propose a supersymmetric model of quark flavor symmetry based on su3colorxsu3wxu1x x t where t binary tetrahedral group is a discrete flavor symmetry group the third heavy generation of quarks are assigned to singlet representation of t while light quark generations are treated differently and assigned to doublet re... | [['we', 'propose', 'a', 'supersymmetric', 'model', 'of', 'quark', 'flavor', 'symmetry', 'based', 'on', 'su3colorxsu3wxu1x', 'x', 't', 'where', 't', 'binary', 'tetrahedral', 'group', 'is', 'a', 'discrete', 'flavor', 'symmetry', 'group', 'the', 'third', 'heavy', 'generation', 'of', 'quarks', 'are', 'assigned', 'to', 'sin... | [-0.09884132876447062, 0.32679551753995856, 0.021906116186088422, 0.08111593961560477, -0.08046175770809859, -0.17715343570609282, 0.0642149920681325, 0.33513047423486303, -0.2184894371331041, -0.2998761923120516, 0.026441766794324223, -0.2949169284202219, 0.030752963575769246, 0.020355878051415813, 0.04388732386079079... |
710.2735 | Effects of polarisation on study of anomalous VVH interactions at a
Linear Collider | We investigate the use of beam polarisation as well as final state $\tau$
polarisation effects in probing the interaction of the Higgs boson with a pair
of heavy vector bosons in the process $e^+ e^- \to f \bar f H$, where $f$ is
any light fermion. The sensitivity of the International Linear Collider (ILC)
operating ... | hep-ph | we investigate the use of beam polarisation as well as final state tau polarisation effects in probing the interaction of the higgs boson with a pair of heavy vector bosons in the process e e to f bar f h where f is any light fermion the sensitivity of the international linear collider ilc operating at sqrt s500 gev to... | [['we', 'investigate', 'the', 'use', 'of', 'beam', 'polarisation', 'as', 'well', 'as', 'final', 'state', 'tau', 'polarisation', 'effects', 'in', 'probing', 'the', 'interaction', 'of', 'the', 'higgs', 'boson', 'with', 'a', 'pair', 'of', 'heavy', 'vector', 'bosons', 'in', 'the', 'process', 'e', 'e', 'to', 'f', 'bar', 'f'... | [-0.11905404391029897, 0.2349604628741359, -0.04690784049065163, 0.10085558555270743, -0.03572199362007758, -0.1779816587551091, -0.0055104041746698125, 0.345743081627939, -0.26675724836949927, -0.26297081472017825, -0.002726440847767756, -0.313702976056494, 0.03537335963203357, 0.13874583378828204, 0.10372470821349476... |
710.2736 | L2 norm performance index of synchronization and optimal control
synthesis of complex networks | In this paper, the synchronizability problem of dynamical networks is
addressed, where better synchronizability means that the network synchronizes
faster with lower-overshoot. The L2 norm of the error vector e is taken as a
performance index to measure this kind of synchronizability. For the
equilibrium synchronizat... | cs.NI | in this paper the synchronizability problem of dynamical networks is addressed where better synchronizability means that the network synchronizes faster with lowerovershoot the l2 norm of the error vector e is taken as a performance index to measure this kind of synchronizability for the equilibrium synchronization cas... | [['in', 'this', 'paper', 'the', 'synchronizability', 'problem', 'of', 'dynamical', 'networks', 'is', 'addressed', 'where', 'better', 'synchronizability', 'means', 'that', 'the', 'network', 'synchronizes', 'faster', 'with', 'lowerovershoot', 'the', 'l2', 'norm', 'of', 'the', 'error', 'vector', 'e', 'is', 'taken', 'as', ... | [-0.16401749148503408, 0.037968414633894144, -0.06729637263715435, 0.07915299211916842, -0.019541463322213872, -0.11283448021004659, 0.04600286560816516, 0.36435708999901795, -0.355824712543286, -0.2550399272481529, 0.10787910482135983, -0.2464543452164788, -0.19329558621100384, 0.12454773039429737, -0.0730019941366539... |
710.2737 | The history of mass assembly of faint red galaxies in 28 galaxy clusters
since z=1.3 | We measure the relative evolution of the number of bright and faint (as faint
as 0.05 L*) red galaxies in a sample of 28 clusters, of which 16 are at 0.50<=
z<=1.27, all observed through a pair of filters bracketing the 4000 Angstrom
break rest-frame. The abundance of red galaxies, relative to bright ones, is
constan... | astro-ph | we measure the relative evolution of the number of bright and faint as faint as 005 l red galaxies in a sample of 28 clusters of which 16 are at 050 z127 all observed through a pair of filters bracketing the 4000 angstrom break restframe the abundance of red galaxies relative to bright ones is constant over all the stu... | [['we', 'measure', 'the', 'relative', 'evolution', 'of', 'the', 'number', 'of', 'bright', 'and', 'faint', 'as', 'faint', 'as', '005', 'l', 'red', 'galaxies', 'in', 'a', 'sample', 'of', '28', 'clusters', 'of', 'which', '16', 'are', 'at', '050', 'z127', 'all', 'observed', 'through', 'a', 'pair', 'of', 'filters', 'bracket... | [-0.044507066590521276, 0.11500301673142634, -0.06506889229837123, 0.08983194664478118, -0.10841465017407424, -0.06466243458701901, 0.08014736237975073, 0.4538377382280961, -0.1299015237674327, -0.3972274175714734, 0.03716211175483743, -0.32951889189720995, 0.027232218761666035, 0.19217421506813556, -0.0468279778576967... |
710.2738 | CdZnTe room-temperature semiconductor operation in liquid scintillator | We demonstrate the first operation of CdZnTe room-temperature detectors in a
liquid scintillator environment. This work follows conceptually the
Heusser-type detector method of operating HPGe detectors in liquid nitrogen and
liquid argon but instead for a far more practical room-temperature ensemble
with the aim of a... | nucl-ex | we demonstrate the first operation of cdznte roomtemperature detectors in a liquid scintillator environment this work follows conceptually the heussertype detector method of operating hpge detectors in liquid nitrogen and liquid argon but instead for a far more practical roomtemperature ensemble with the aim of achievi... | [['we', 'demonstrate', 'the', 'first', 'operation', 'of', 'cdznte', 'roomtemperature', 'detectors', 'in', 'a', 'liquid', 'scintillator', 'environment', 'this', 'work', 'follows', 'conceptually', 'the', 'heussertype', 'detector', 'method', 'of', 'operating', 'hpge', 'detectors', 'in', 'liquid', 'nitrogen', 'and', 'liqui... | [-0.053445379334209744, 0.20230238287545302, -0.06858257339427284, -0.06286964764106362, 0.07863415790466118, -0.2196422536839165, 0.06350279803953919, 0.42195071104694815, -0.1299018556909526, -0.3595188652329585, 0.05398305429273522, -0.36850111179199874, -0.052290136834570004, 0.21035154208120907, -0.038762175615000... |
710.2739 | The look-ahead effect of phenotypic mutations | The evolution of complex molecular traits such as disulphide bridges often
requires multiple mutations. The intermediate steps in such evolutionary
trajectories are likely to be selectively neutral or deleterious. Therefore,
large populations and long times may be required to evolve such traits. We
propose that error... | q-bio.PE | the evolution of complex molecular traits such as disulphide bridges often requires multiple mutations the intermediate steps in such evolutionary trajectories are likely to be selectively neutral or deleterious therefore large populations and long times may be required to evolve such traits we propose that errors in t... | [['the', 'evolution', 'of', 'complex', 'molecular', 'traits', 'such', 'as', 'disulphide', 'bridges', 'often', 'requires', 'multiple', 'mutations', 'the', 'intermediate', 'steps', 'in', 'such', 'evolutionary', 'trajectories', 'are', 'likely', 'to', 'be', 'selectively', 'neutral', 'or', 'deleterious', 'therefore', 'large... | [-0.07971190008935412, 0.164589784249074, -0.07819944966203449, 0.14702758827214976, -0.08096704166911711, -0.2098123618052341, 0.13419636670005275, 0.3979545397874476, -0.2798173173108477, -0.22730122007223227, 0.062243964269741395, -0.17309691135200078, -0.1862311624685059, 0.1526360279663508, -0.11472588280131193, -... |
710.274 | Reliability of Module Based Software System | This paper consider the problem of determining the reliability of a software
system which can be decomposed in a number of modules. We have derived the
expression of the reliability of a system using the Markovian model for the
transfer of control between modules in order. We have given the expression of
reliability ... | stat.AP | this paper consider the problem of determining the reliability of a software system which can be decomposed in a number of modules we have derived the expression of the reliability of a system using the markovian model for the transfer of control between modules in order we have given the expression of reliability by c... | [['this', 'paper', 'consider', 'the', 'problem', 'of', 'determining', 'the', 'reliability', 'of', 'a', 'software', 'system', 'which', 'can', 'be', 'decomposed', 'in', 'a', 'number', 'of', 'modules', 'we', 'have', 'derived', 'the', 'expression', 'of', 'the', 'reliability', 'of', 'a', 'system', 'using', 'the', 'markovian... | [-0.16237579744220823, 0.0103074788418879, -0.051686835116201854, 0.02880281040933073, -0.001875341477164303, -0.12466157835919454, 0.047156558732547045, 0.3306444350585162, -0.25662590070145136, -0.34321556352527743, 0.14315802920525558, -0.1984736396740359, -0.16241927467376352, 0.21582518739861448, -0.10275088874510... |
710.2741 | Dark Energy, Induced Gravity and Broken Scale Invariance | We study the cosmological evolution of an induced gravity model with a
self-interacting scalar field $\sigma$ and in the presence of matter and
radiation. Such model leads to Einstein Gravity plus a cosmological constant as
a stable attractor among homogeneous cosmologies and is therefore a viable
dark-energy (DE) mo... | astro-ph gr-qc hep-th | we study the cosmological evolution of an induced gravity model with a selfinteracting scalar field sigma and in the presence of matter and radiation such model leads to einstein gravity plus a cosmological constant as a stable attractor among homogeneous cosmologies and is therefore a viable darkenergy de model for a ... | [['we', 'study', 'the', 'cosmological', 'evolution', 'of', 'an', 'induced', 'gravity', 'model', 'with', 'a', 'selfinteracting', 'scalar', 'field', 'sigma', 'and', 'in', 'the', 'presence', 'of', 'matter', 'and', 'radiation', 'such', 'model', 'leads', 'to', 'einstein', 'gravity', 'plus', 'a', 'cosmological', 'constant', ... | [-0.19548636827040727, 0.1647115440362438, -0.1140270132938741, 0.08327090688554806, -0.12391278808477374, -0.1887029321129683, -0.08859003672841936, 0.28186576356980164, -0.198253312161271, -0.3091373388773539, 0.04393434533554221, -0.22369393146216449, -0.08358870981864526, 0.14939632315621515, 0.044068845428368995, ... |
710.2742 | Relic gravitons from super-inflation | The super-inflationary phase is predicted by the Loop Quantum Cosmology. In
this paper we study the creation of gravitational waves during this phase. We
consider the inverse volume corrections to the equation for the tensor modes
and calculate the spectrum of the produced gravitons. The amplitude of the
obtained spe... | gr-qc | the superinflationary phase is predicted by the loop quantum cosmology in this paper we study the creation of gravitational waves during this phase we consider the inverse volume corrections to the equation for the tensor modes and calculate the spectrum of the produced gravitons the amplitude of the obtained spectrum ... | [['the', 'superinflationary', 'phase', 'is', 'predicted', 'by', 'the', 'loop', 'quantum', 'cosmology', 'in', 'this', 'paper', 'we', 'study', 'the', 'creation', 'of', 'gravitational', 'waves', 'during', 'this', 'phase', 'we', 'consider', 'the', 'inverse', 'volume', 'corrections', 'to', 'the', 'equation', 'for', 'the', '... | [-0.1463764483574778, 0.22448092870569478, -0.10703307461226359, 0.09784039893808465, -0.058809660173331696, -0.04732231035983811, 0.017242307767931682, 0.2746224887048205, -0.2254150689036275, -0.28377369010510545, 0.11075044704484753, -0.2305153656518087, -0.12831187616102396, 0.1644299962363827, -0.00964213739304492... |
710.2743 | Non-minimal coupling as a mechanism for spontaneous symmetry breaking on
the brane | Motivated by the dimensional asymmetry characteristic of braneworlds, we
populate the bulk spacetime with matter scalar fields, both real and complex,
and couple them non-minimally to gravity. We derive the effective equations of
motion on the brane and realize the case when the fields acquire a
non-vanishing vacuum ... | hep-th | motivated by the dimensional asymmetry characteristic of braneworlds we populate the bulk spacetime with matter scalar fields both real and complex and couple them nonminimally to gravity we derive the effective equations of motion on the brane and realize the case when the fields acquire a nonvanishing vacuum expectat... | [['motivated', 'by', 'the', 'dimensional', 'asymmetry', 'characteristic', 'of', 'braneworlds', 'we', 'populate', 'the', 'bulk', 'spacetime', 'with', 'matter', 'scalar', 'fields', 'both', 'real', 'and', 'complex', 'and', 'couple', 'them', 'nonminimally', 'to', 'gravity', 'we', 'derive', 'the', 'effective', 'equations', ... | [-0.16779757553067443, 0.20881545814363478, -0.04635521985381563, 0.11248645272484555, -0.09917853180771675, -0.12553101735381045, -0.023843316030558025, 0.2944796796818481, -0.2105520310557108, -0.32481658416060366, 0.04113019636840882, -0.22653331740968208, -0.08667614516175448, 0.1319036965006005, 0.0289369398449486... |
710.2744 | Electromagnetic form factors of the Delta baryon | We develop a methodology that enables us to extract accurately the
electromagnetic Delta form factors and their momentum dependence. We test our
approach in the quenched approximation as a preparation for a study using
dynamical fermions. Our calculation of the four form factors covers pion masses
between about 410 M... | hep-lat hep-ph nucl-th | we develop a methodology that enables us to extract accurately the electromagnetic delta form factors and their momentum dependence we test our approach in the quenched approximation as a preparation for a study using dynamical fermions our calculation of the four form factors covers pion masses between about 410 mev a... | [['we', 'develop', 'a', 'methodology', 'that', 'enables', 'us', 'to', 'extract', 'accurately', 'the', 'electromagnetic', 'delta', 'form', 'factors', 'and', 'their', 'momentum', 'dependence', 'we', 'test', 'our', 'approach', 'in', 'the', 'quenched', 'approximation', 'as', 'a', 'preparation', 'for', 'a', 'study', 'using'... | [-0.09915266663799238, 0.15857531117092774, -0.08474985785527617, 0.06217575823872262, -0.045512364296198815, -0.058178222094439604, 0.1168908600990947, 0.37319533385209036, -0.1871060337871313, -0.33222818578808355, 0.022176488783234395, -0.3069773060070653, -0.06415633142440237, 0.16910954350685206, 0.048120327898834... |
710.2745 | Two-dimensional multisolitons and azimuthons in Bose-Einstein
condensates with attraction | We present spatially localized nonrotating and rotating (azimuthon)
multisolitons in the two-dimensional (2D) ("pancake-shaped configuration")
Bose-Einstein condensate (BEC) with attractive interaction. By means of a
linear stability analysis, we investigate the stability of these structures and
show that rotating di... | nlin.PS | we present spatially localized nonrotating and rotating azimuthon multisolitons in the twodimensional 2d pancakeshaped configuration boseeinstein condensate bec with attractive interaction by means of a linear stability analysis we investigate the stability of these structures and show that rotating dipole solitons are... | [['we', 'present', 'spatially', 'localized', 'nonrotating', 'and', 'rotating', 'azimuthon', 'multisolitons', 'in', 'the', 'twodimensional', '2d', 'pancakeshaped', 'configuration', 'boseeinstein', 'condensate', 'bec', 'with', 'attractive', 'interaction', 'by', 'means', 'of', 'a', 'linear', 'stability', 'analysis', 'we',... | [-0.20155597384884738, 0.1637777433730662, -0.030842897611168714, 0.04521385446513215, -0.0018534267464509378, -0.12899575459126097, -0.03763384123404439, 0.3719732509782681, -0.18082852504717617, -0.2248120475273866, 0.052751838983609696, -0.2562878134445502, -0.1336331281381158, 0.16549838153430477, 0.100509417529862... |
710.2746 | Kullback Leibler property of kernel mixture priors in Bayesian density
estimation | Positivity of the prior probability of Kullback-Leibler neighborhood around
the true density, commonly known as the Kullback-Leibler property, plays a
fundamental role in posterior consistency. A popular prior for Bayesian
estimation is given by a Dirichlet mixture, where the kernels are chosen
depending on the sampl... | math.ST stat.TH | positivity of the prior probability of kullbackleibler neighborhood around the true density commonly known as the kullbackleibler property plays a fundamental role in posterior consistency a popular prior for bayesian estimation is given by a dirichlet mixture where the kernels are chosen depending on the sample space ... | [['positivity', 'of', 'the', 'prior', 'probability', 'of', 'kullbackleibler', 'neighborhood', 'around', 'the', 'true', 'density', 'commonly', 'known', 'as', 'the', 'kullbackleibler', 'property', 'plays', 'a', 'fundamental', 'role', 'in', 'posterior', 'consistency', 'a', 'popular', 'prior', 'for', 'bayesian', 'estimatio... | [-0.05181972689752001, 0.06552243874175474, -0.13433285076753237, 0.13783831895998447, -0.07936027855612338, -0.1291913531080354, 0.02809223501899396, 0.39332682981621475, -0.2823203982785344, -0.2564092840446392, 0.1215952534788812, -0.19507606802653754, -0.10849221863172716, 0.177443624647276, -0.10756299717177172, 0... |
710.2747 | Simulations of the consequences of tongue surgery on tongue mobility:
implications for speech production in post-surgery conditions | This paper presents simulations of the impact of tongue surgery on tongue
movements and on speech articulation. For this, a 3D biomechanical Finite
Element (FE) model of the tongue is used. Muscles are represented within the FE
structure by specific subsets of elements. The tongue model is inserted in the
upper airwa... | physics.med-ph | this paper presents simulations of the impact of tongue surgery on tongue movements and on speech articulation for this a 3d biomechanical finite element fe model of the tongue is used muscles are represented within the fe structure by specific subsets of elements the tongue model is inserted in the upper airways inclu... | [['this', 'paper', 'presents', 'simulations', 'of', 'the', 'impact', 'of', 'tongue', 'surgery', 'on', 'tongue', 'movements', 'and', 'on', 'speech', 'articulation', 'for', 'this', 'a', '3d', 'biomechanical', 'finite', 'element', 'fe', 'model', 'of', 'the', 'tongue', 'is', 'used', 'muscles', 'are', 'represented', 'within... | [-0.07087084309371765, 0.11461564445290977, -0.034809299009281515, 0.04629840932681527, -0.02156159323869719, -0.12526929800556055, -0.028754442767895967, 0.404418930811414, -0.22838137109278583, -0.30628220980796755, 0.10340861538359501, -0.3059651994238227, -0.1703221519366169, 0.20875585388267595, -0.137161107581358... |
710.2748 | Algebraic curves for commuting elements in the q-deformed Heisenberg
algebra | In this paper we extend the eliminant construction of Burchnall and Chaundy
for commuting differential operators in the Heisenberg algebra to the
q-deformed Heisenberg algebra and show that it again provides annihilating
curves for commuting elements, provided q satisfies a natural condition. As a
side result we obta... | math.RA math.QA | in this paper we extend the eliminant construction of burchnall and chaundy for commuting differential operators in the heisenberg algebra to the qdeformed heisenberg algebra and show that it again provides annihilating curves for commuting elements provided q satisfies a natural condition as a side result we obtain es... | [['in', 'this', 'paper', 'we', 'extend', 'the', 'eliminant', 'construction', 'of', 'burchnall', 'and', 'chaundy', 'for', 'commuting', 'differential', 'operators', 'in', 'the', 'heisenberg', 'algebra', 'to', 'the', 'qdeformed', 'heisenberg', 'algebra', 'and', 'show', 'that', 'it', 'again', 'provides', 'annihilating', 'c... | [-0.1635471096387439, 0.06625076056694362, -0.0809714819179542, 0.02915247572488638, -0.09354525451798604, -0.10093569230816479, -0.01823301763280726, 0.2964045757170655, -0.31745479219773814, -0.1671707849643791, 0.10155424487658901, -0.2774769558168169, -0.13930691875962178, 0.219314117860327, -0.1286412863505643, -0... |
710.2749 | Coupling of Surface and Volume Dipole Oscillations in C-60 Molecules | We first give a short review of the ``local-current approximation'' (LCA),
derived from a general variation principle, which serves as a semiclassical
description of strongly collective excitations in finite fermion systems
starting from their quantum-mechanical mean-field ground state. We illustrate
it for the examp... | physics.atm-clus nucl-th physics.atom-ph physics.flu-dyn | we first give a short review of the localcurrent approximation lca derived from a general variation principle which serves as a semiclassical description of strongly collective excitations in finite fermion systems starting from their quantummechanical meanfield ground state we illustrate it for the example of coupled ... | [['we', 'first', 'give', 'a', 'short', 'review', 'of', 'the', 'localcurrent', 'approximation', 'lca', 'derived', 'from', 'a', 'general', 'variation', 'principle', 'which', 'serves', 'as', 'a', 'semiclassical', 'description', 'of', 'strongly', 'collective', 'excitations', 'in', 'finite', 'fermion', 'systems', 'starting'... | [-0.1276648123621602, 0.18232738238505342, -0.10664966608482328, 0.06858047184280373, -0.027146345819346607, -0.09471432143314318, 0.07021318405697291, 0.36332848044112326, -0.18860390525395898, -0.244618194330145, -0.05748652979646894, -0.3175244712609459, -0.15221118466632272, 0.13098062023478138, 0.04494862018830397... |
710.275 | Transition from galactic to extragalactic cosmic rays | The transition from galactic to extragalactic cosmic rays is discussed. One
of critical indications for transition is given by the Standard Model of
Galactic cosmic rays, according to which the maximum energy of acceleration for
iron nuclei is of order of $E_{\rm Fe}^{\rm max} \approx 1\times 10^{17}$ eV.
At $E > E_{... | astro-ph | the transition from galactic to extragalactic cosmic rays is discussed one of critical indications for transition is given by the standard model of galactic cosmic rays according to which the maximum energy of acceleration for iron nuclei is of order of e_rm ferm max approx 1times 1017 ev at e e_rm ferm max the spectru... | [['the', 'transition', 'from', 'galactic', 'to', 'extragalactic', 'cosmic', 'rays', 'is', 'discussed', 'one', 'of', 'critical', 'indications', 'for', 'transition', 'is', 'given', 'by', 'the', 'standard', 'model', 'of', 'galactic', 'cosmic', 'rays', 'according', 'to', 'which', 'the', 'maximum', 'energy', 'of', 'accelera... | [-0.018041834678484622, 0.253304331433272, 0.028156798500181317, 0.11342147606481924, 0.006290891459903082, -0.08370161814184038, 0.03313690370892268, 0.3941987953291124, -0.23666140037348826, -0.41314569671178747, -0.01447632947914286, -0.3737261928958558, 0.04076481776161518, 0.1718784422424569, 0.05104177215799494, ... |
710.2751 | A note on mean volume and surface densities for a class of
birth-and-growth stochastic processes | Many real phenomena may be modelled as locally finite unions of
$d$-dimensional time dependent random closed sets in $\mathbb{R}^d$, described
by birth-and-growth stochastic processes, so that their mean volume and surface
densities, as well as the so called mean \emph{extended} volume and surface
densities, may be s... | math.PR | many real phenomena may be modelled as locally finite unions of ddimensional time dependent random closed sets in mathbbrd described by birthandgrowth stochastic processes so that their mean volume and surface densities as well as the so called mean emphextended volume and surface densities may be studied in terms of r... | [['many', 'real', 'phenomena', 'may', 'be', 'modelled', 'as', 'locally', 'finite', 'unions', 'of', 'ddimensional', 'time', 'dependent', 'random', 'closed', 'sets', 'in', 'mathbbrd', 'described', 'by', 'birthandgrowth', 'stochastic', 'processes', 'so', 'that', 'their', 'mean', 'volume', 'and', 'surface', 'densities', 'a... | [-0.0798389099297985, 0.18991578912602797, -0.04841761445371254, 0.10085307236617917, -0.007002158761425044, -0.06058513628499162, 0.0441370335925791, 0.3397322313769931, -0.30655448631413523, -0.23881411135336886, 0.11214722338463029, -0.2189863235839913, -0.14850747507686415, 0.21285389745307545, -0.09474654546788623... |
710.2752 | Future plan for observation of cosmic gamma rays in the 100 TeV energy
region with the Tibet air shower array : simulation and sensitivity | The Tibet air shower array, which has an effective area of 37,000 square
meters and is located at 4300 m in altitude, has been observing air showers
induced by cosmic rays with energies above a few TeV. We have a plan to add a
large muon detector array to it for the purpose of increasing its sensitivity
to cosmic gam... | astro-ph | the tibet air shower array which has an effective area of 37000 square meters and is located at 4300 m in altitude has been observing air showers induced by cosmic rays with energies above a few tev we have a plan to add a large muon detector array to it for the purpose of increasing its sensitivity to cosmic gamma ray... | [['the', 'tibet', 'air', 'shower', 'array', 'which', 'has', 'an', 'effective', 'area', 'of', '37000', 'square', 'meters', 'and', 'is', 'located', 'at', '4300', 'm', 'in', 'altitude', 'has', 'been', 'observing', 'air', 'showers', 'induced', 'by', 'cosmic', 'rays', 'with', 'energies', 'above', 'a', 'few', 'tev', 'we', 'h... | [-0.06305223279678733, 0.23628286128569195, -0.04797411799467731, 0.10154340691555587, -0.0054744422657064876, -0.02450810808061373, -0.004948570826413608, 0.45537248095220856, -0.2008372664331726, -0.4466829967712707, 0.0580174050104832, -0.38664504288151713, 0.03080463591999937, 0.22161067720032343, 0.065729688481591... |
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