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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707.173 | Can Strong Gravitational Lensing Constrain Dark Energy? | We discuss the ratio of the angular diameter distances from the source to the
lens, $D_{ds}$, and to the observer at present, $D_{s}$, for various dark
energy models. It is well known that the difference of $D_s$s between the
models is apparent and this quantity is used for the analysis of Type Ia
supernovae. However... | astro-ph | we discuss the ratio of the angular diameter distances from the source to the lens d_ds and to the observer at present d_s for various dark energy models it is well known that the difference of d_ss between the models is apparent and this quantity is used for the analysis of type ia supernovae however we investigate th... | [['we', 'discuss', 'the', 'ratio', 'of', 'the', 'angular', 'diameter', 'distances', 'from', 'the', 'source', 'to', 'the', 'lens', 'd_ds', 'and', 'to', 'the', 'observer', 'at', 'present', 'd_s', 'for', 'various', 'dark', 'energy', 'models', 'it', 'is', 'well', 'known', 'that', 'the', 'difference', 'of', 'd_ss', 'between... | [-0.10927317691599264, 0.0838448230676246, -0.10179407849939068, 0.13078583767815855, -0.0854722065126978, -0.098274808802584, -0.007565049013974029, 0.36371984459352835, -0.24773967776583444, -0.35667998235200365, 0.05849309584502416, -0.267733355843725, -0.04266028351408906, 0.2153576215301333, -0.0017205783897138013... |
707.1731 | A purely reflective large wide-field telescope | Two versions of a fast, purely reflective Paul-Baker type telescope are
discussed, each with an 8.4-m aperture, 3 deg diameter flat field and f/1.25
focal ratio.
The first version is based on a common, even asphere type of surface with
zero conic constant. The primary and tertiary mirrors are 6th order aspheres,
wh... | astro-ph | two versions of a fast purely reflective paulbaker type telescope are discussed each with an 84m aperture 3 deg diameter flat field and f125 focal ratio the first version is based on a common even asphere type of surface with zero conic constant the primary and tertiary mirrors are 6th order aspheres while the secondar... | [['two', 'versions', 'of', 'a', 'fast', 'purely', 'reflective', 'paulbaker', 'type', 'telescope', 'are', 'discussed', 'each', 'with', 'an', '84m', 'aperture', '3', 'deg', 'diameter', 'flat', 'field', 'and', 'f125', 'focal', 'ratio', 'the', 'first', 'version', 'is', 'based', 'on', 'a', 'common', 'even', 'asphere', 'type... | [-0.11965150866258921, 0.08146574402900181, -0.050918185165267714, 0.0028283178910223695, -0.08529833665033434, -0.14690763425045136, -0.012045320043192998, 0.3853493254121372, -0.20474101856645555, -0.32104137138526695, 0.1400261619799155, -0.2983512138358533, -0.09236166435478013, 0.2020191770667831, -0.0910791453055... |
707.1732 | The Two-Spectra Inverse Problem for Semi-Infinite Jacobi Matrices in The
Limit-Circle Case | We present a technique for reconstructing a semi-infinite Jacobi operator in
the limit circle case from the spectra of two different self-adjoint
extensions. Moreover, we give necessary and sufficient conditions for two real
sequences to be the spectra of two different self-adjoint extensions of a
Jacobi operator in ... | math-ph math.MP | we present a technique for reconstructing a semiinfinite jacobi operator in the limit circle case from the spectra of two different selfadjoint extensions moreover we give necessary and sufficient conditions for two real sequences to be the spectra of two different selfadjoint extensions of a jacobi operator in the lim... | [['we', 'present', 'a', 'technique', 'for', 'reconstructing', 'a', 'semiinfinite', 'jacobi', 'operator', 'in', 'the', 'limit', 'circle', 'case', 'from', 'the', 'spectra', 'of', 'two', 'different', 'selfadjoint', 'extensions', 'moreover', 'we', 'give', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'two', 'real'... | [-0.15045032377999562, 0.07957528214543484, -0.06463199510024144, 0.09443515720060812, -0.05225560842350555, -0.1457131016605462, -0.04013080287796374, 0.370821168502936, -0.2633527202818256, -0.19246672831762296, 0.14855812292528123, -0.2949256217107177, -0.13607704026911122, 0.2115844009229197, -0.0514850145778977, 0... |
707.1733 | Cyclotomic $q$-Schur algebras associated to the Ariki-Koike algebra | Let $S$ be the cyclotomic $q$-Schur algebra associated to the Ariki-Koike
algebra $H_{n,r}$ of rank $n$, introduced by Dipper-James-Mathas. For each $p =
(r_1, ..., r_g)$ such that $r_1 + ... + r_g = r$, we define a subalgebra $S^p$
of $S$ and its quotient algebra $\bar S^p$. It is shown that $S^p$ is a
standardly ba... | math.RT math.QA | let s be the cyclotomic qschur algebra associated to the arikikoike algebra h_nr of rank n introduced by dipperjamesmathas for each p r_1 r_g such that r_1 r_g r we define a subalgebra sp of s and its quotient algebra bar sp it is shown that sp is a standardly based algebra and bar sp is a cellular algebra by making us... | [['let', 's', 'be', 'the', 'cyclotomic', 'qschur', 'algebra', 'associated', 'to', 'the', 'arikikoike', 'algebra', 'h_nr', 'of', 'rank', 'n', 'introduced', 'by', 'dipperjamesmathas', 'for', 'each', 'p', 'r_1', 'r_g', 'such', 'that', 'r_1', 'r_g', 'r', 'we', 'define', 'a', 'subalgebra', 'sp', 'of', 's', 'and', 'its', 'qu... | [-0.20741626448386039, 0.0846141535995735, -0.07593710671903359, 0.07072316509438678, -0.11007025220638347, -0.19284945824183525, -0.06633711396199134, 0.3282118268724945, -0.4309024409287506, -0.1576455047974984, 0.13106385093803208, -0.20127406699789896, -0.13874387613032013, 0.18172898883931338, -0.10816049384884537... |
707.1734 | Kinematic fast cosmic dynamos in non-inflationary phases of ellipsoidal
universe | Cosmic kinematic fast dynamo is found in non-inflationary phases of an
ellipsoidal anisotropic cosmological metric background solution of Einstein
field equations of general relativity. The magnetic field is amplified inside
the universe and spatially periodically. A finite resistivity is assumed, and a
nonsingular f... | gr-qc | cosmic kinematic fast dynamo is found in noninflationary phases of an ellipsoidal anisotropic cosmological metric background solution of einstein field equations of general relativity the magnetic field is amplified inside the universe and spatially periodically a finite resistivity is assumed and a nonsingular flow ve... | [['cosmic', 'kinematic', 'fast', 'dynamo', 'is', 'found', 'in', 'noninflationary', 'phases', 'of', 'an', 'ellipsoidal', 'anisotropic', 'cosmological', 'metric', 'background', 'solution', 'of', 'einstein', 'field', 'equations', 'of', 'general', 'relativity', 'the', 'magnetic', 'field', 'is', 'amplified', 'inside', 'the'... | [-0.2224919154908355, 0.2125204830353303, -0.08910957357386919, 0.07710044312191974, -0.13044460205846045, -0.06130008331869971, -0.10664334668449368, 0.3307846053774558, -0.24032289890113145, -0.2467323152527009, 0.054638633814685, -0.2154683773979953, -0.08405183891650952, 0.18082858955213316, -0.002805888031953021, ... |
707.1735 | Finite Anomalous Magnetic Moment in the Gauge-Higgs Unification | We show that the anomalous magnetic moment of fermion in the gauge-Higgs
unification is finite in any spacetime dimensions, which is a new predictive
physical observable similar to the Higgs mass.
| hep-ph | we show that the anomalous magnetic moment of fermion in the gaugehiggs unification is finite in any spacetime dimensions which is a new predictive physical observable similar to the higgs mass | [['we', 'show', 'that', 'the', 'anomalous', 'magnetic', 'moment', 'of', 'fermion', 'in', 'the', 'gaugehiggs', 'unification', 'is', 'finite', 'in', 'any', 'spacetime', 'dimensions', 'which', 'is', 'a', 'new', 'predictive', 'physical', 'observable', 'similar', 'to', 'the', 'higgs', 'mass']] | [-0.13843262940645218, 0.26978752443627, -0.07876764391098291, 0.17152199405245483, -0.12990554169781746, -0.14892970264378574, -0.028316306872218245, 0.33396561744232334, -0.17055175986681734, -0.26058547904775026, 0.020069289947352974, -0.1787804932964425, -0.09326907307390243, 0.10800532816398528, -0.037697397292621... |
707.1736 | Spiral Wave Solutions of One-dimensional Ginzburg-Landau Equation By
Extended F-expansion Method | The one-dimensional Ginzburg-Landau (GL) Equation is considered. We use the
recently developed extended F-expansion method to obtain spiral wave solution
of one-dimensional GL Equation.
| nlin.SI | the onedimensional ginzburglandau gl equation is considered we use the recently developed extended fexpansion method to obtain spiral wave solution of onedimensional gl equation | [['the', 'onedimensional', 'ginzburglandau', 'gl', 'equation', 'is', 'considered', 'we', 'use', 'the', 'recently', 'developed', 'extended', 'fexpansion', 'method', 'to', 'obtain', 'spiral', 'wave', 'solution', 'of', 'onedimensional', 'gl', 'equation']] | [-0.15452938371648392, -0.035922750170963504, -0.12906237614030638, 0.08503783931276605, -0.21563769900240004, -0.14386481659797332, -0.02239021115625898, 0.27128871406118077, -0.22259381972253323, -0.2131790705025196, 0.07678759491924818, -0.21965568947295347, -0.2186826163281997, 0.1603692057542503, 0.092438946943730... |
707.1737 | Conformal invariant powers of the Laplacian, Fefferman-Graham ambient
metric and Ricci gauging | The hierarchy of conformally invariant k-th powers of the Laplacian acting on
a scalar field with scaling dimensions $\Delta_{(k)}=k-d/2$, k=1,2,3 as
obtained in the recent work [1] is rederived using the Fefferman-Graham d+2
dimensional ambient space approach. The corresponding mysterious "holographic"
structure of ... | hep-th | the hierarchy of conformally invariant kth powers of the laplacian acting on a scalar field with scaling dimensions delta_kkd2 k123 as obtained in the recent work 1 is rederived using the feffermangraham d2 dimensional ambient space approach the corresponding mysterious holographic structure of these operators is clari... | [['the', 'hierarchy', 'of', 'conformally', 'invariant', 'kth', 'powers', 'of', 'the', 'laplacian', 'acting', 'on', 'a', 'scalar', 'field', 'with', 'scaling', 'dimensions', 'delta_kkd2', 'k123', 'as', 'obtained', 'in', 'the', 'recent', 'work', '1', 'is', 'rederived', 'using', 'the', 'feffermangraham', 'd2', 'dimensional... | [-0.15323036724841724, 0.1327914218818869, -0.06989689703570098, 0.06937849316846138, -0.10220705668982719, -0.15622067773934975, -0.06453929280722014, 0.329982258179175, -0.19424461032093693, -0.24045553567108288, 0.09219045155826876, -0.2390497094320674, -0.18536413602671156, 0.10818767806975751, -0.00935021265139502... |
707.1738 | Fields of invariants of finite linear groups | The survey is devoted to the rationality question of finite linear groups. We
concentrate on lower-dimensional cases, especially on the case of dimension
four.
| math.AG | the survey is devoted to the rationality question of finite linear groups we concentrate on lowerdimensional cases especially on the case of dimension four | [['the', 'survey', 'is', 'devoted', 'to', 'the', 'rationality', 'question', 'of', 'finite', 'linear', 'groups', 'we', 'concentrate', 'on', 'lowerdimensional', 'cases', 'especially', 'on', 'the', 'case', 'of', 'dimension', 'four']] | [-0.15471935563255101, 0.02417602021402369, -0.0007863730813066164, 0.07569516002452777, -0.08632847743380505, -0.06898811964007716, 0.031648834235966206, 0.3221859303303063, -0.20776173458822692, -0.20185466824720302, 0.17324318645114545, -0.2987851856354003, -0.1321060643143331, 0.22731972792341062, -0.09382196546842... |
707.1739 | On slow-fading non-separable correlation MIMO systems | In a frequency selective slow-fading channel in a MIMO system, the channel
matrix is of the form of a block matrix. We propose a method to calculate the
limit of the eigenvalue distribution of block matrices if the size of the
blocks tends to infinity. We will also calculate the asymptotic eigenvalue
distribution of ... | cs.IT math.IT | in a frequency selective slowfading channel in a mimo system the channel matrix is of the form of a block matrix we propose a method to calculate the limit of the eigenvalue distribution of block matrices if the size of the blocks tends to infinity we will also calculate the asymptotic eigenvalue distribution of hh whe... | [['in', 'a', 'frequency', 'selective', 'slowfading', 'channel', 'in', 'a', 'mimo', 'system', 'the', 'channel', 'matrix', 'is', 'of', 'the', 'form', 'of', 'a', 'block', 'matrix', 'we', 'propose', 'a', 'method', 'to', 'calculate', 'the', 'limit', 'of', 'the', 'eigenvalue', 'distribution', 'of', 'block', 'matrices', 'if',... | [-0.1354818135337985, 0.08560212941792207, -0.09725282614564766, 0.01342102346293952, -0.03608341126945679, -0.1294708009161379, 0.047952759743708634, 0.3574947012993305, -0.2915034690932573, -0.2314852226647022, 0.12080186049089484, -0.2643347507909588, -0.15611658634860878, 0.08869679020515278, -0.04347421414745243, ... |
707.174 | The Generation and Dissipation of Interstellar Turbulence - Results from
Large Scale High Resolution Simulations | We study, by means of adaptive mesh refinement hydro- and
magnetohydrodynamical simulations that cover a wide range of scales (from kpc
to sub-parsec), the dimension of the most dissipative structures and the
injection scale of the turbulent interstellar gas, which we find to be about 75
pc, in agreement with observa... | astro-ph | we study by means of adaptive mesh refinement hydro and magnetohydrodynamical simulations that cover a wide range of scales from kpc to subparsec the dimension of the most dissipative structures and the injection scale of the turbulent interstellar gas which we find to be about 75 pc in agreement with observations this... | [['we', 'study', 'by', 'means', 'of', 'adaptive', 'mesh', 'refinement', 'hydro', 'and', 'magnetohydrodynamical', 'simulations', 'that', 'cover', 'a', 'wide', 'range', 'of', 'scales', 'from', 'kpc', 'to', 'subparsec', 'the', 'dimension', 'of', 'the', 'most', 'dissipative', 'structures', 'and', 'the', 'injection', 'scale... | [-0.10503175087340128, 0.16110824964079953, -0.06672254053680876, 0.04715472795570074, -0.03806846811934266, -0.051362654043978814, 0.0022318102954074653, 0.37439959046300936, -0.2486927635124397, -0.34558834060809984, 0.07308090762722544, -0.2504677190147557, -0.01949316929202787, 0.19472705103662732, 0.01084320156342... |
707.1741 | Computer Simulation of Host and two Parasite Species with Ageing | The possible coexistence of one host, one aggressive parasite and one
non-lethal parasite is simulated using the Penna model of biological ageing. If
the aggressive parasites survive the difficult initial times where they have to
adjust genetically to the proper host age, all three species may survive,
though the hos... | q-bio.PE | the possible coexistence of one host one aggressive parasite and one nonlethal parasite is simulated using the penna model of biological ageing if the aggressive parasites survive the difficult initial times where they have to adjust genetically to the proper host age all three species may survive though the host numbe... | [['the', 'possible', 'coexistence', 'of', 'one', 'host', 'one', 'aggressive', 'parasite', 'and', 'one', 'nonlethal', 'parasite', 'is', 'simulated', 'using', 'the', 'penna', 'model', 'of', 'biological', 'ageing', 'if', 'the', 'aggressive', 'parasites', 'survive', 'the', 'difficult', 'initial', 'times', 'where', 'they', ... | [-0.08598656552554719, 0.23875478326728375, -0.0480718236850125, 0.10381401926961503, -0.06875277147628367, -0.24003919702151727, 0.08450124668085883, 0.3587652970233868, -0.252809462009062, -0.3012170644862385, 0.1295193998817483, -0.255004581802621, -0.12795935481272894, 0.13021504239516396, -0.11373335569454678, -0.... |
707.1742 | Relative log convergent cohomology and relative rigid cohomology I | In this paper, we develop the theory of relative log convergent cohomology.
We prove the coherence of relative log convergent cohomology in certain case by
using the comparison theorem between relative log convergent cohomlogy and
relative log crystalline cohomology, and we relates relative log convergent
cohomology ... | math.NT math.AG | in this paper we develop the theory of relative log convergent cohomology we prove the coherence of relative log convergent cohomology in certain case by using the comparison theorem between relative log convergent cohomlogy and relative log crystalline cohomology and we relates relative log convergent cohomology to re... | [['in', 'this', 'paper', 'we', 'develop', 'the', 'theory', 'of', 'relative', 'log', 'convergent', 'cohomology', 'we', 'prove', 'the', 'coherence', 'of', 'relative', 'log', 'convergent', 'cohomology', 'in', 'certain', 'case', 'by', 'using', 'the', 'comparison', 'theorem', 'between', 'relative', 'log', 'convergent', 'coh... | [-0.17933197010314048, 0.036843977768772414, -0.15354530962871477, 0.07180866770241187, -0.02620577852108649, -0.1189456163972084, 0.025534141158762697, 0.3344548582431993, -0.34117328297967714, -0.25160510663685964, 0.04014924938313752, -0.2050864393351644, -0.11073895428507101, 0.1861140714248731, -0.266063104228427,... |
707.1743 | Relative log convergent cohomology and relative rigid cohomology II | In this paper, we develop the theory of relative log convergent cohomology of
radius $\lambda$ ($0 < \lambda \leq 1$), which is a generalization of the
notion of relative log convergent cohomology in the previous paper. By
comparing this cohomology with relative log crystalline cohomology, relative
rigid cohomology a... | math.NT math.AG | in this paper we develop the theory of relative log convergent cohomology of radius lambda 0 lambda leq 1 which is a generalization of the notion of relative log convergent cohomology in the previous paper by comparing this cohomology with relative log crystalline cohomology relative rigid cohomology and its variants a... | [['in', 'this', 'paper', 'we', 'develop', 'the', 'theory', 'of', 'relative', 'log', 'convergent', 'cohomology', 'of', 'radius', 'lambda', '0', 'lambda', 'leq', '1', 'which', 'is', 'a', 'generalization', 'of', 'the', 'notion', 'of', 'relative', 'log', 'convergent', 'cohomology', 'in', 'the', 'previous', 'paper', 'by', '... | [-0.17965122567489744, 0.03357025032863021, -0.13389410926649967, 0.019629428912885487, -0.016153036803007125, -0.11373704273874562, 0.011803023306808123, 0.31317746100326377, -0.3446042861416936, -0.26869230685134726, 0.058620859791214265, -0.20055322182364763, -0.12535231319566567, 0.15431923830260832, -0.22719689150... |
707.1744 | Statistical properties of a generalized threshold network model | The threshold network model is a type of finite random graphs. In this paper,
we introduce a generalized threshold network model. A pair of vertices with
random weights is connected by an edge when real-valued functions of the pair
of weights belong to given Borel sets. We extend several known limit theorems
for the ... | math.PR | the threshold network model is a type of finite random graphs in this paper we introduce a generalized threshold network model a pair of vertices with random weights is connected by an edge when realvalued functions of the pair of weights belong to given borel sets we extend several known limit theorems for the number ... | [['the', 'threshold', 'network', 'model', 'is', 'a', 'type', 'of', 'finite', 'random', 'graphs', 'in', 'this', 'paper', 'we', 'introduce', 'a', 'generalized', 'threshold', 'network', 'model', 'a', 'pair', 'of', 'vertices', 'with', 'random', 'weights', 'is', 'connected', 'by', 'an', 'edge', 'when', 'realvalued', 'functi... | [-0.14849386916362814, 0.1226527080942192, -0.05133584267016323, 0.06882741357271914, -0.060143793118186295, -0.11724220130348667, 0.08275266844430007, 0.3553697688593751, -0.31151712173596025, -0.22466389745906262, 0.065939598105615, -0.27261308260217665, -0.15801452251062506, 0.14669962396423908, -0.07917429315247795... |
707.1745 | On the Graf's addition theorem for Hahn Exton q-Bessel function | In this paper we study the positivity of the generalized $q$-translation
associated with the $q$-Bessel Hahn Exton function which is deduced by a new
formulation of the Graf's addition formula related to this function.
| math.CA | in this paper we study the positivity of the generalized qtranslation associated with the qbessel hahn exton function which is deduced by a new formulation of the grafs addition formula related to this function | [['in', 'this', 'paper', 'we', 'study', 'the', 'positivity', 'of', 'the', 'generalized', 'qtranslation', 'associated', 'with', 'the', 'qbessel', 'hahn', 'exton', 'function', 'which', 'is', 'deduced', 'by', 'a', 'new', 'formulation', 'of', 'the', 'grafs', 'addition', 'formula', 'related', 'to', 'this', 'function']] | [-0.08804629669722283, 0.047520539822113336, -0.10962676618135336, 0.07880253224478413, -0.06868818695798065, -0.05474388468163935, 0.022851778663497305, 0.2683864146696799, -0.3027386349259001, -0.2384426129812544, 0.08051781621267737, -0.21450851019471884, -0.26361011442813004, 0.17742707931690596, -0.105473373734364... |
707.1746 | Random environment on coloured trees | In this paper, we study a regular rooted coloured tree with random labels
assigned to its edges, where the distribution of the label assigned to an edge
depends on the colours of its endpoints. We obtain some new results relevant to
this model and also show how our model generalizes many other probabilistic
models, i... | math.PR | in this paper we study a regular rooted coloured tree with random labels assigned to its edges where the distribution of the label assigned to an edge depends on the colours of its endpoints we obtain some new results relevant to this model and also show how our model generalizes many other probabilistic models includi... | [['in', 'this', 'paper', 'we', 'study', 'a', 'regular', 'rooted', 'coloured', 'tree', 'with', 'random', 'labels', 'assigned', 'to', 'its', 'edges', 'where', 'the', 'distribution', 'of', 'the', 'label', 'assigned', 'to', 'an', 'edge', 'depends', 'on', 'the', 'colours', 'of', 'its', 'endpoints', 'we', 'obtain', 'some', '... | [-0.061536712711838644, 0.16835274533938596, -0.061209197233741484, 0.04217645740168842, -0.1165758128109802, -0.14929143510784748, 0.11694556827973833, 0.42497412643084925, -0.27631516655674204, -0.2239195640043666, 0.06620684439096497, -0.2995904023345146, -0.18049174009097946, 0.09690381464315578, -0.129589683612317... |
707.1747 | Charmed Exotics in Heavy Ion Collisions | Based on the color-spin interaction in diquarks, we argue that charmed
multiquark hadrons are likely to exist. Because of the appreciable number of
charm quarks produced in central nucleus-nucleus collisions at
ultrarelativistic energies, production of charmed multiquark hadrons is
expected to be enhanced in these co... | hep-ph | based on the colorspin interaction in diquarks we argue that charmed multiquark hadrons are likely to exist because of the appreciable number of charm quarks produced in central nucleusnucleus collisions at ultrarelativistic energies production of charmed multiquark hadrons is expected to be enhanced in these collision... | [['based', 'on', 'the', 'colorspin', 'interaction', 'in', 'diquarks', 'we', 'argue', 'that', 'charmed', 'multiquark', 'hadrons', 'are', 'likely', 'to', 'exist', 'because', 'of', 'the', 'appreciable', 'number', 'of', 'charm', 'quarks', 'produced', 'in', 'central', 'nucleusnucleus', 'collisions', 'at', 'ultrarelativistic... | [-0.03748893975231719, 0.37170423539161374, -0.16210791520037068, 0.22775140905893446, -0.01330833999478879, -0.103626787851681, 0.02041530191975956, 0.33898748251764727, -0.13349454479854708, -0.20772078975763483, -0.1345938083929165, -0.39994044577664073, 0.1333460106028118, 0.01811858513390992, 0.13781149526281902, ... |
707.1748 | Algebraic Connections vs. Algebraic {$\cD$}-modules: inverse and direct
images | In the dictionary between the language of (algebraic integrable) connections
and that of (algebraic) $\cD$-modules, to compare the definitions of inverse
images for connections and $\cD$-modules is easy. But the comparison between
direct images for connections (the classical construction of the Gauss-Manin
connection... | math.AG | in the dictionary between the language of algebraic integrable connections and that of algebraic cdmodules to compare the definitions of inverse images for connections and cdmodules is easy but the comparison between direct images for connections the classical construction of the gaussmanin connection for smooth morphi... | [['in', 'the', 'dictionary', 'between', 'the', 'language', 'of', 'algebraic', 'integrable', 'connections', 'and', 'that', 'of', 'algebraic', 'cdmodules', 'to', 'compare', 'the', 'definitions', 'of', 'inverse', 'images', 'for', 'connections', 'and', 'cdmodules', 'is', 'easy', 'but', 'the', 'comparison', 'between', 'dire... | [-0.11056445009023996, 0.012062415506966871, -0.12313462065237506, 0.1145198614941342, -0.13200044925267831, -0.1386546792275068, 0.03734097508401269, 0.3511023516596363, -0.29795586451797224, -0.28160743174574726, 0.08332387132502002, -0.22274142976498185, -0.1842841497770079, 0.19568890519298204, -0.15918272321975632... |
707.1749 | New results from the B factories Belle and BaBar | The BELLE detector has already accumulated e^+ e^- collision data at the
KEKB-collider corresponding to 600 fb^-1. BaBar has accumulated data of
approximately 390 fb^-1 at PEP-II. Both are running on asymmetric energy e^+
e^- colliders at the Upsilon(4S) energy. The paper selects important results
from both experimen... | hep-ex | the belle detector has already accumulated e e collision data at the kekbcollider corresponding to 600 fb1 babar has accumulated data of approximately 390 fb1 at pepii both are running on asymmetric energy e e colliders at the upsilon4s energy the paper selects important results from both experiments with the emphasis ... | [['the', 'belle', 'detector', 'has', 'already', 'accumulated', 'e', 'e', 'collision', 'data', 'at', 'the', 'kekbcollider', 'corresponding', 'to', '600', 'fb1', 'babar', 'has', 'accumulated', 'data', 'of', 'approximately', '390', 'fb1', 'at', 'pepii', 'both', 'are', 'running', 'on', 'asymmetric', 'energy', 'e', 'e', 'co... | [-0.10335295702407166, 0.14874526658786635, -0.07717490867798915, 0.07264226622646675, -0.09259871459653368, -0.14592633164284052, 0.05353941002613283, 0.30786153284134343, -0.14857724588364363, -0.3221522578969598, 0.004220373119096621, -0.5088311968502239, 0.11532661138335243, 0.173593675968732, 0.12733170711726416, ... |
707.175 | The accuracy of roughness exponent measurement methods | We test methods for measuring and characterizing rough profiles with emphasis
on measurements of the self-affine roughness exponent, and describes a simple
test to separate between roughness exponents originating from long range
correlations in the sign signs of the profile, and roughness exponents
originating from L... | cond-mat.stat-mech cond-mat.mtrl-sci | we test methods for measuring and characterizing rough profiles with emphasis on measurements of the selfaffine roughness exponent and describes a simple test to separate between roughness exponents originating from long range correlations in the sign signs of the profile and roughness exponents originating from levy d... | [['we', 'test', 'methods', 'for', 'measuring', 'and', 'characterizing', 'rough', 'profiles', 'with', 'emphasis', 'on', 'measurements', 'of', 'the', 'selfaffine', 'roughness', 'exponent', 'and', 'describes', 'a', 'simple', 'test', 'to', 'separate', 'between', 'roughness', 'exponents', 'originating', 'from', 'long', 'ran... | [-0.0641710278320989, 0.11635665984915718, -0.14516689768346724, 0.09879645562382197, 0.0028324040882089434, -0.12506046172151444, 0.04176600330132146, 0.37720813486507976, -0.2393680555357432, -0.34289954531869277, 0.07045612127185896, -0.3422111142426729, -0.09978868584919927, 0.26207285991475626, -0.0178878855908666... |
707.1751 | Thermodynamics and superfluid density in BCS-BEC crossover with and
without population imbalance | We address the thermodynamics, density profiles and superfluid density of
trapped fermions undergoing BCS-BEC crossover, with and without population
imbalance. Our approach represents a fully consistent treatment of "pseudogap
effects", which reflect the distinction between the pair formation temperature
$T^*$ and th... | cond-mat.str-el cond-mat.quant-gas cond-mat.supr-con | we address the thermodynamics density profiles and superfluid density of trapped fermions undergoing bcsbec crossover with and without population imbalance our approach represents a fully consistent treatment of pseudogap effects which reflect the distinction between the pair formation temperature t and the pair conden... | [['we', 'address', 'the', 'thermodynamics', 'density', 'profiles', 'and', 'superfluid', 'density', 'of', 'trapped', 'fermions', 'undergoing', 'bcsbec', 'crossover', 'with', 'and', 'without', 'population', 'imbalance', 'our', 'approach', 'represents', 'a', 'fully', 'consistent', 'treatment', 'of', 'pseudogap', 'effects'... | [-0.11305790529298163, 0.15504123603990663, -0.11960159919170428, 0.062271474037789605, -0.03053419028173734, -0.1138285274608332, 0.07853433066126846, 0.347345129930351, -0.19665461169438236, -0.3118742395698735, 0.015085185601068571, -0.3245318782000432, -0.09273201911212894, 0.13200832333458695, -0.02955074559612362... |
707.1752 | Large amplitude oscillatory motion along a solar filament | Large amplitude oscillations of solar filaments is a phenomenon known for
more than half a century. Recently, a new mode of oscillations, characterized
by periodical plasma motions along the filament axis, was discovered. We
analyze such an event, recorded on 23 January 2002 in Big Bear Solar
Observatory H$\alpha$ fi... | astro-ph | large amplitude oscillations of solar filaments is a phenomenon known for more than half a century recently a new mode of oscillations characterized by periodical plasma motions along the filament axis was discovered we analyze such an event recorded on 23 january 2002 in big bear solar observatory halpha filtergrams i... | [['large', 'amplitude', 'oscillations', 'of', 'solar', 'filaments', 'is', 'a', 'phenomenon', 'known', 'for', 'more', 'than', 'half', 'a', 'century', 'recently', 'a', 'new', 'mode', 'of', 'oscillations', 'characterized', 'by', 'periodical', 'plasma', 'motions', 'along', 'the', 'filament', 'axis', 'was', 'discovered', 'w... | [-0.1924427532172326, 0.17521191035766412, -0.036493623052584995, 0.04969789125124349, -0.06899208684669847, -0.05454042244088301, 0.0006859232721097291, 0.35469041314927185, -0.25222882960942833, -0.35071683855766944, 0.08329001772787145, -0.24371315004493535, -0.09355814989502641, 0.21362796813606263, -0.000830199433... |
707.1753 | On decomposition numbers with Jantzen filtration of cyclotomic $q$-Schur
algebras | Let $\Sc(\vL)$ be the cyclotomic $q$-Schur algebra associated to the
Ariki-Koike algebra $\He_{n,r}$, introduced by Dipper-James-Mathas. In this
paper, we consider $v$-decomposition numbers of $\Sc(\vL)$, namely
decomposition numbers with respect to the Jantzen filtrations of Weyl modules.
We prove, as a $v$-analogue... | math.RT math.QA | let scvl be the cyclotomic qschur algebra associated to the arikikoike algebra he_nr introduced by dipperjamesmathas in this paper we consider vdecomposition numbers of scvl namely decomposition numbers with respect to the jantzen filtrations of weyl modules we prove as a vanalogue of the result obtained by shojiwada a... | [['let', 'scvl', 'be', 'the', 'cyclotomic', 'qschur', 'algebra', 'associated', 'to', 'the', 'arikikoike', 'algebra', 'he_nr', 'introduced', 'by', 'dipperjamesmathas', 'in', 'this', 'paper', 'we', 'consider', 'vdecomposition', 'numbers', 'of', 'scvl', 'namely', 'decomposition', 'numbers', 'with', 'respect', 'to', 'the',... | [-0.2221825616136986, 0.09795418935530681, -0.06432088415950854, 0.07697686729234386, -0.08021837593294046, -0.13896989994286063, -0.021796060378039057, 0.26211416408261085, -0.3717959419764737, -0.21800595222528965, 0.09742699094745826, -0.17982894858466758, -0.15676164987715, 0.2402849596469326, -0.16881361529429226,... |
707.1754 | Emission Line Variability of the Accreting Young Brown Dwarf 2MASSW
J1207334-393254: From Hours to Years | We have obtained a series of high-resolution optical spectra for the brown
dwarf 2MASSW J1207334-393254 (2M1207) using the ESO Very Large Telescope with
the UVES spectrograph during two consecutive observing nights (time resolution
of ~12 min) and the Magellan Clay telescope with the MIKE spectrograph.
Combined with ... | astro-ph | we have obtained a series of highresolution optical spectra for the brown dwarf 2massw j1207334393254 2m1207 using the eso very large telescope with the uves spectrograph during two consecutive observing nights time resolution of 12 min and the magellan clay telescope with the mike spectrograph combined with previously... | [['we', 'have', 'obtained', 'a', 'series', 'of', 'highresolution', 'optical', 'spectra', 'for', 'the', 'brown', 'dwarf', '2massw', 'j1207334393254', '2m1207', 'using', 'the', 'eso', 'very', 'large', 'telescope', 'with', 'the', 'uves', 'spectrograph', 'during', 'two', 'consecutive', 'observing', 'nights', 'time', 'resol... | [-0.1140816639222869, 0.13419800365740872, -0.05757633226184065, 0.05700361586230643, -0.10715300578843145, -0.10264043090865016, 0.046730512611889825, 0.4433588414617321, -0.17059933910059044, -0.3852567616028382, 0.10956725984536153, -0.2728243468890843, -0.008691902352010776, 0.25584655380996135, -0.0548928274536806... |
707.1755 | Coupling to a phononic mode in $Bi_{2-x}Pb_xSr_2CaCu_2O_{8+\delta}$:
Angle-resolved photoemission | The kink in the dispersion and the drop in the width observed by
angle-resolved photoemission in the nodal direction of the Brillouin zone of
$\mathrm{Bi_{2-x}Pb_xSr_2CaCu_2O_{8+ \delta}}$ (abbreviated as (Pb)Bi2212) has
attracted broad interest [1-3]. Surprisingly optimally lead-doped (Pb)Bi2212
with $\mathrm{T_C>89... | cond-mat.supr-con | the kink in the dispersion and the drop in the width observed by angleresolved photoemission in the nodal direction of the brillouin zone of mathrmbi_2xpb_xsr_2cacu_2o_8 delta abbreviated as pbbi2212 has attracted broad interest 13 surprisingly optimally leaddoped pbbi2212 with mathrmt_c89k as well as the shadow band w... | [['the', 'kink', 'in', 'the', 'dispersion', 'and', 'the', 'drop', 'in', 'the', 'width', 'observed', 'by', 'angleresolved', 'photoemission', 'in', 'the', 'nodal', 'direction', 'of', 'the', 'brillouin', 'zone', 'of', 'mathrmbi_2xpb_xsr_2cacu_2o_8', 'delta', 'abbreviated', 'as', 'pbbi2212', 'has', 'attracted', 'broad', 'i... | [-0.14632753830913697, 0.13274684652608387, -0.05637955430105234, 0.08645907503956504, -0.06669092972326694, -0.10584713267074025, 0.08358835483476802, 0.3828408404834026, -0.28365388034866484, -0.3147313536404149, 0.08745099384414291, -0.2906733997625924, -0.11627321051362949, 0.206653715305832, 0.011905875708318399, ... |
707.1756 | On the divisor function and the Riemann zeta-function in short intervals | We obtain, for $T^\epsilon \le U=U(T)\le T^{1/2-\epsilon}$, asymptotic
formulas for $$ \int_T^{2T}(E(t+U) - E(t))^2 dt,\quad \int_T^{2T}(\Delta(t+U) -
\Delta(t))^2 dt, $$ where $\Delta(x)$ is the error term in the classical
divisor problem, and $E(T)$ is the error term in the mean square formula for
$|\zeta(1/2+it)|$... | math.NT | we obtain for tepsilon le uutle t12epsilon asymptotic formulas for int_t2tetu et2 dtquad int_t2tdeltatu deltat2 dt where deltax is the error term in the classical divisor problem and et is the error term in the mean square formula for zeta12it upper bounds of the form o_epsilont1epsilonu2 for the above integrals with b... | [['we', 'obtain', 'for', 'tepsilon', 'le', 'uutle', 't12epsilon', 'asymptotic', 'formulas', 'for', 'int_t2tetu', 'et2', 'dtquad', 'int_t2tdeltatu', 'deltat2', 'dt', 'where', 'deltax', 'is', 'the', 'error', 'term', 'in', 'the', 'classical', 'divisor', 'problem', 'and', 'et', 'is', 'the', 'error', 'term', 'in', 'the', 'm... | [-0.14054617130364302, 0.08826846816795475, -0.022513463334352883, 0.12506252177559804, -0.04846693779468352, -0.14063853502595497, 0.03649768086127293, 0.2917654534778845, -0.26592305997087634, -0.2723139919179641, 0.12037470518973553, -0.34443637634409063, -0.13685686915917436, 0.24447350926053377, -0.086018057843852... |
707.1757 | Coalescence of Rotating Black Holes on Eguchi-Hanson Space | We obtain new charged rotating multi-black hole solutions on the
Eguchi-Hanson space in the five-dimensional Einstein-Maxwell system with a
Chern-Simons term and a positive cosmological constant. In the two-black holes
case, these solutions describe the coalescence of two rotating black holes with
the spatial topolog... | hep-th gr-qc | we obtain new charged rotating multiblack hole solutions on the eguchihanson space in the fivedimensional einsteinmaxwell system with a chernsimons term and a positive cosmological constant in the twoblack holes case these solutions describe the coalescence of two rotating black holes with the spatial topologies of s3 ... | [['we', 'obtain', 'new', 'charged', 'rotating', 'multiblack', 'hole', 'solutions', 'on', 'the', 'eguchihanson', 'space', 'in', 'the', 'fivedimensional', 'einsteinmaxwell', 'system', 'with', 'a', 'chernsimons', 'term', 'and', 'a', 'positive', 'cosmological', 'constant', 'in', 'the', 'twoblack', 'holes', 'case', 'these',... | [-0.21639191611326364, 0.07625654869649595, -0.03517220246162519, 0.12149523036753379, -0.05739623633692566, -0.13376940636289786, -0.032821503639655206, 0.2782188841295474, -0.13456680846301097, -0.2830580024645456, 0.1036131272953709, -0.33098929499285024, -0.08491772979280902, 0.15403726210510268, -0.031017778387058... |
707.1758 | Track Reconstruction and Performance of DRIFT Directional Dark Matter
Detectors using Alpha Particles | First results are presented from an analysis of data from the DRIFT-IIa and
DRIFT-IIb directional dark matter detectors at Boulby Mine in which alpha
particle tracks were reconstructed and used to characterise detector
performance--an important step towards optimising directional technology. The
drift velocity in DRI... | physics.ins-det | first results are presented from an analysis of data from the driftiia and driftiib directional dark matter detectors at boulby mine in which alpha particle tracks were reconstructed and used to characterise detector performancean important step towards optimising directional technology the drift velocity in driftiia w... | [['first', 'results', 'are', 'presented', 'from', 'an', 'analysis', 'of', 'data', 'from', 'the', 'driftiia', 'and', 'driftiib', 'directional', 'dark', 'matter', 'detectors', 'at', 'boulby', 'mine', 'in', 'which', 'alpha', 'particle', 'tracks', 'were', 'reconstructed', 'and', 'used', 'to', 'characterise', 'detector', 'p... | [-0.005787171744224098, 0.18814579440923235, -0.05353918858648588, 0.04269652302480406, 0.033493040581406265, -0.11918363908254025, -0.0006582476095192962, 0.3356511028552497, -0.17926204835789072, -0.40590665936470033, 0.060771248733228145, -0.3769249345072442, 0.01651081278644226, 0.2044545137875334, -0.0152641100442... |
707.1759 | Torsional shear oscillations in the neutron star crust driven by
restoring force of elastic stresses | We present several exact solutions of the eigenfrequency problem for
torsional shear vibrations in homogeneous and non-homogeneous models of the
neutron star crust governed by canonical equation of solid mechanics with a
restoring force of Hookean elasticity. Particular attention is given to regime
of large lengthsca... | astro-ph | we present several exact solutions of the eigenfrequency problem for torsional shear vibrations in homogeneous and nonhomogeneous models of the neutron star crust governed by canonical equation of solid mechanics with a restoring force of hookean elasticity particular attention is given to regime of large lengthscale n... | [['we', 'present', 'several', 'exact', 'solutions', 'of', 'the', 'eigenfrequency', 'problem', 'for', 'torsional', 'shear', 'vibrations', 'in', 'homogeneous', 'and', 'nonhomogeneous', 'models', 'of', 'the', 'neutron', 'star', 'crust', 'governed', 'by', 'canonical', 'equation', 'of', 'solid', 'mechanics', 'with', 'a', 'r... | [-0.18426596095355657, 0.19167547708090682, -0.04224902932317211, 0.05015286102873058, -0.13346061947074933, -0.09120867823322232, 0.012566545790132996, 0.3273379790525024, -0.26118626340578954, -0.2663511907395262, 0.05938714568753942, -0.2320505799439091, -0.10504756257332001, 0.21720117892926702, -0.0318426937263351... |
707.176 | E_0-dilation of strongly commuting CP_0-semigroups | We prove that every strongly commuting pair of CP_0-semigroups has a minimal
E_0-dilation. This is achieved in two major steps, interesting in themselves:
1: we show that a strongly commuting pair of CP_0-semigroups can be represented
via a two parameter product system representation; 2: we prove that every fully
coi... | math.OA | we prove that every strongly commuting pair of cp_0semigroups has a minimal e_0dilation this is achieved in two major steps interesting in themselves 1 we show that a strongly commuting pair of cp_0semigroups can be represented via a two parameter product system representation 2 we prove that every fully coisometric pr... | [['we', 'prove', 'that', 'every', 'strongly', 'commuting', 'pair', 'of', 'cp_0semigroups', 'has', 'a', 'minimal', 'e_0dilation', 'this', 'is', 'achieved', 'in', 'two', 'major', 'steps', 'interesting', 'in', 'themselves', '1', 'we', 'show', 'that', 'a', 'strongly', 'commuting', 'pair', 'of', 'cp_0semigroups', 'can', 'be... | [-0.1890808693314721, 0.16857745999930723, -0.062164978753146416, -0.0016760768780073561, -0.006372784116220745, -0.16954690546958479, -0.0470654574742952, 0.4095769029461428, -0.2902115087036963, -0.1527002065974687, 0.08223361141114895, -0.295442435624344, -0.16148788665645067, 0.17379080037308203, -0.081561553594353... |
707.1761 | On Excess of the Odious Primes | We give a more strong heuristic justification of our conjecture on the excess
of the odious primes.
| math.NT | we give a more strong heuristic justification of our conjecture on the excess of the odious primes | [['we', 'give', 'a', 'more', 'strong', 'heuristic', 'justification', 'of', 'our', 'conjecture', 'on', 'the', 'excess', 'of', 'the', 'odious', 'primes']] | [-0.17901336562628037, -0.024594586726058933, -0.21475274882772388, 0.16859529474202326, -0.11014406514518402, -0.10710056539734497, 0.13201843399335356, 0.29186900529791326, -0.14277183220666997, -0.29469117456499266, -0.013365480637944797, -0.25804217593908746, -0.1206867738681681, 0.2045459138941677, -0.115786023711... |
707.1762 | Continuous Opinion Dynamics under Bounded Confidence: A Survey | Models of continuous opinion dynamics under bounded confidence have been
presented independently by Krause and Hegselmann and by Deffuant et al in 2000.
They have raised a fair amount of attention in the communities of social
simulation, sociophysics and complexity science. The researchers working on it
come from dis... | physics.soc-ph math.DS nlin.AO | models of continuous opinion dynamics under bounded confidence have been presented independently by krause and hegselmann and by deffuant et al in 2000 they have raised a fair amount of attention in the communities of social simulation sociophysics and complexity science the researchers working on it come from discipli... | [['models', 'of', 'continuous', 'opinion', 'dynamics', 'under', 'bounded', 'confidence', 'have', 'been', 'presented', 'independently', 'by', 'krause', 'and', 'hegselmann', 'and', 'by', 'deffuant', 'et', 'al', 'in', '2000', 'they', 'have', 'raised', 'a', 'fair', 'amount', 'of', 'attention', 'in', 'the', 'communities', '... | [-0.054848446947756535, 0.1161676474764724, -0.10161655532186203, 0.08374381241485736, -0.12416512954959785, -0.15249106947936175, 0.06680707630195859, 0.4099465932716979, -0.27207526711517954, -0.3197881700969077, 0.10047035643713857, -0.28019478105202833, -0.1522377275657606, 0.13904307613194108, -0.09740615669976581... |
707.1763 | The two dimensional spin and its resonance fringe | Violation of Bell's Inequalities gives experimental evidence for the
existence of a spin 1/2 which has two simultaneous axes of spin quantization
rather than one. These couple to form a resonance state, called the spin
fringe, and this quantum effect is solely responsible for violation of Bell's
Inequalities within t... | physics.gen-ph | violation of bells inequalities gives experimental evidence for the existence of a spin 12 which has two simultaneous axes of spin quantization rather than one these couple to form a resonance state called the spin fringe and this quantum effect is solely responsible for violation of bells inequalities within this mode... | [['violation', 'of', 'bells', 'inequalities', 'gives', 'experimental', 'evidence', 'for', 'the', 'existence', 'of', 'a', 'spin', '12', 'which', 'has', 'two', 'simultaneous', 'axes', 'of', 'spin', 'quantization', 'rather', 'than', 'one', 'these', 'couple', 'to', 'form', 'a', 'resonance', 'state', 'called', 'the', 'spin'... | [-0.13540580826987214, 0.19039061932411608, -0.08540884775816868, 0.10050624297417805, -0.04193913224943966, -0.20251644632058605, 0.018379820582131803, 0.3116801050667352, -0.21692731461137915, -0.2990588276067151, 0.0430388109437805, -0.2833991986787263, -0.08795698377180775, 0.1936817263947132, 0.0010614863812115113... |
707.1764 | Spin structure function g_1 at small x and arbitrary $Q^2: Total
resummaion of leading logarithms vs Standard Approach | The Standard Approach (SA) for description of the structure function g_1
combines the DGLAP evolution equations and Standard Fits for the initial parton
densities. The DGLAP equations describe the region of large Q^2 and large x, so
there are not theoretical grounds to exploit them at small x. In practice,
extrapolat... | hep-ph | the standard approach sa for description of the structure function g_1 combines the dglap evolution equations and standard fits for the initial parton densities the dglap equations describe the region of large q2 and large x so there are not theoretical grounds to exploit them at small x in practice extrapolation of dg... | [['the', 'standard', 'approach', 'sa', 'for', 'description', 'of', 'the', 'structure', 'function', 'g_1', 'combines', 'the', 'dglap', 'evolution', 'equations', 'and', 'standard', 'fits', 'for', 'the', 'initial', 'parton', 'densities', 'the', 'dglap', 'equations', 'describe', 'the', 'region', 'of', 'large', 'q2', 'and',... | [-0.053724754411329435, 0.1110832205498203, -0.1532574311592422, 0.159686396699423, -0.0624120911306818, -0.07673815930320416, 0.004538955865427852, 0.35460234114240546, -0.22133685511895843, -0.24373780697351322, 0.05259455109019958, -0.26233380820121965, -0.013722058505663881, 0.15412632979253735, -0.0147645418286022... |
707.1765 | On the discriminant of elliptic curves with non-trivial torsion | For those elliptic curves defined over the rational with non--trivial torsion
subgroup, we find a tight relationship between the torsion subgroup itself and
a Galois group naturally arising from the curve.
| math.NT | for those elliptic curves defined over the rational with nontrivial torsion subgroup we find a tight relationship between the torsion subgroup itself and a galois group naturally arising from the curve | [['for', 'those', 'elliptic', 'curves', 'defined', 'over', 'the', 'rational', 'with', 'nontrivial', 'torsion', 'subgroup', 'we', 'find', 'a', 'tight', 'relationship', 'between', 'the', 'torsion', 'subgroup', 'itself', 'and', 'a', 'galois', 'group', 'naturally', 'arising', 'from', 'the', 'curve']] | [-0.27725710449439867, 0.05909943534812379, -0.17019228571124614, 0.08487961561449113, -0.18833396328432905, -0.13374069227927154, 0.03688413145080689, 0.333002406360221, -0.44634261366821104, -0.2934889440094271, 0.03299161251033506, -0.27443156102972643, -0.1516517069896743, 0.2928499045871919, -0.1661194520852258, -... |
707.1766 | Harmonic analysis on local fields and adelic spaces I | We develop a harmonic analysis on objects of some category $C_2$ of
infinite-dimensional filtered vector spaces over a finite field. It includes
two-dimensional local fields and adelic spaces of algebraic surfaces defined
over a finite field. The main result is the theory of the Fourier transform on
these objects and... | math.AG math.NT | we develop a harmonic analysis on objects of some category c_2 of infinitedimensional filtered vector spaces over a finite field it includes twodimensional local fields and adelic spaces of algebraic surfaces defined over a finite field the main result is the theory of the fourier transform on these objects and twodime... | [['we', 'develop', 'a', 'harmonic', 'analysis', 'on', 'objects', 'of', 'some', 'category', 'c_2', 'of', 'infinitedimensional', 'filtered', 'vector', 'spaces', 'over', 'a', 'finite', 'field', 'it', 'includes', 'twodimensional', 'local', 'fields', 'and', 'adelic', 'spaces', 'of', 'algebraic', 'surfaces', 'defined', 'over... | [-0.1637918156536542, 0.09680598470786551, -0.13444960887438423, 0.10514759839257612, -0.09146845569166373, -0.06440945864953804, -0.01831904905277111, 0.3736883611681889, -0.31846479769304115, -0.16144194940702533, 0.10771286899645655, -0.18743336130425614, -0.1638749004605244, 0.2699940412773153, -0.11789191585283436... |
707.1767 | The spectral data for Hamiltonian stationary Lagrangian tori in R^4 | This article determines the spectral data, in the integrable systems sense,
for all weakly conformally immersed Hamiltonian stationary Lagrangian in
$\R^4$. This enables us to describe their moduli space and the locus of branch
points of such an immersion. This is also an informative example in integrable
systems geo... | math.DG math.SG | this article determines the spectral data in the integrable systems sense for all weakly conformally immersed hamiltonian stationary lagrangian in r4 this enables us to describe their moduli space and the locus of branch points of such an immersion this is also an informative example in integrable systems geometry sinc... | [['this', 'article', 'determines', 'the', 'spectral', 'data', 'in', 'the', 'integrable', 'systems', 'sense', 'for', 'all', 'weakly', 'conformally', 'immersed', 'hamiltonian', 'stationary', 'lagrangian', 'in', 'r4', 'this', 'enables', 'us', 'to', 'describe', 'their', 'moduli', 'space', 'and', 'the', 'locus', 'of', 'bran... | [-0.17005477889211146, 0.11454788072060419, -0.09123766092982676, 0.073499949210529, -0.0882915052730445, -0.09795660281239392, -0.022396075478815412, 0.3470183276123815, -0.265750307567847, -0.23833068871459404, 0.11709724152732834, -0.2601333357417932, -0.16953441421440862, 0.185185738706163, -0.1356780425427699, 0.0... |
707.1768 | Greybody factors in a rotating black-hole background-II : fermions and
gauge bosons | We study the emission of fermion and gauge boson degrees of freedom on the
brane by a rotating higher-dimensional black hole. Using matching techniques,
for the near-horizon and far-field regime solutions, we solve analytically the
corresponding field equations of motion. From this, we derive analytical
results for t... | hep-th hep-ph | we study the emission of fermion and gauge boson degrees of freedom on the brane by a rotating higherdimensional black hole using matching techniques for the nearhorizon and farfield regime solutions we solve analytically the corresponding field equations of motion from this we derive analytical results for the absorpt... | [['we', 'study', 'the', 'emission', 'of', 'fermion', 'and', 'gauge', 'boson', 'degrees', 'of', 'freedom', 'on', 'the', 'brane', 'by', 'a', 'rotating', 'higherdimensional', 'black', 'hole', 'using', 'matching', 'techniques', 'for', 'the', 'nearhorizon', 'and', 'farfield', 'regime', 'solutions', 'we', 'solve', 'analytica... | [-0.09406439514141383, 0.1242536723267243, -0.060867770391655716, 0.11272492405947473, -0.03751561064896445, -0.12180351290492503, 0.056233884546700426, 0.3557292423394369, -0.15544798137715424, -0.28000697386487733, 0.04807901376671356, -0.3185561654207436, -0.09513515115561565, 0.19555926949379776, 0.0180384934527843... |
707.1769 | Magnetospectroscopy of symmetric and anti-symmetric states in double
quantum wells | The experimental results obtained for the magneto-transport in the
InGaAs/InAlAs double quantum wells (DQW) structures of two different shapes of
wells are reported. The beating-effect occurred in the Shubnikov-de Haas (SdH)
oscillations was observed for both types of the structures at low temperatures
in the paralle... | cond-mat.str-el | the experimental results obtained for the magnetotransport in the ingaasinalas double quantum wells dqw structures of two different shapes of wells are reported the beatingeffect occurred in the shubnikovde haas sdh oscillations was observed for both types of the structures at low temperatures in the parallel transport... | [['the', 'experimental', 'results', 'obtained', 'for', 'the', 'magnetotransport', 'in', 'the', 'ingaasinalas', 'double', 'quantum', 'wells', 'dqw', 'structures', 'of', 'two', 'different', 'shapes', 'of', 'wells', 'are', 'reported', 'the', 'beatingeffect', 'occurred', 'in', 'the', 'shubnikovde', 'haas', 'sdh', 'oscillat... | [-0.176518585582669, 0.2166071621398308, -0.06760670277218953, 0.08202931214522087, -0.008809042129423897, -0.147740978399249, 0.005740743823605412, 0.3554256080173468, -0.24555715741163106, -0.3422794563923287, 0.0021831606095301286, -0.28962029391572675, -0.14695769314519094, 0.23330655208440454, 0.034568283013743525... |
707.177 | Quantum Monte Carlo results for bipolaron stability in quantum dots | Bipolaron formation in a two-dimensional lattice with harmonic confinement,
representing a simplified model for a quantum dot, is investigated by means of
quantum Monte Carlo simulations. This method treats all interactions exactly
and takes into account quantum lattice fluctuations. Calculations of the
bipolaron bin... | cond-mat.str-el cond-mat.mtrl-sci | bipolaron formation in a twodimensional lattice with harmonic confinement representing a simplified model for a quantum dot is investigated by means of quantum monte carlo simulations this method treats all interactions exactly and takes into account quantum lattice fluctuations calculations of the bipolaron binding en... | [['bipolaron', 'formation', 'in', 'a', 'twodimensional', 'lattice', 'with', 'harmonic', 'confinement', 'representing', 'a', 'simplified', 'model', 'for', 'a', 'quantum', 'dot', 'is', 'investigated', 'by', 'means', 'of', 'quantum', 'monte', 'carlo', 'simulations', 'this', 'method', 'treats', 'all', 'interactions', 'exac... | [-0.19176190485829822, 0.20969624076615614, -0.07070454486719151, 0.10897635262580993, -0.018895516025266894, -0.19679713774593952, 0.08135007781675085, 0.3293732713740926, -0.25437592494341993, -0.29535749998024624, -0.05007315575494431, -0.26052308908623195, -0.07090503806577307, 0.1382246986588301, 0.109416529758954... |
707.1771 | On long-time dynamics for competition-diffusion systems with
inhomogeneous Dirichlet boundary conditions | We consider a two-component competition-diffusion system with equal diffusion
coefficients and inhomogeneous Dirichlet boundary conditions. When the
interspecific competition parameter tends to infinity, the system solution
converges to that of a freeboundary problem. If all stationary solutions of
this limit problem... | math.AP | we consider a twocomponent competitiondiffusion system with equal diffusion coefficients and inhomogeneous dirichlet boundary conditions when the interspecific competition parameter tends to infinity the system solution converges to that of a freeboundary problem if all stationary solutions of this limit problem are no... | [['we', 'consider', 'a', 'twocomponent', 'competitiondiffusion', 'system', 'with', 'equal', 'diffusion', 'coefficients', 'and', 'inhomogeneous', 'dirichlet', 'boundary', 'conditions', 'when', 'the', 'interspecific', 'competition', 'parameter', 'tends', 'to', 'infinity', 'the', 'system', 'solution', 'converges', 'to', '... | [-0.15366618313884828, 0.15091512432671153, -0.045204265862703326, 0.04107243836275302, -0.08863837987184525, -0.23548497372772545, -0.017861938951537013, 0.282924409636762, -0.31352535702288153, -0.17336007830686867, 0.1847722058184445, -0.3220006835833192, -0.09226747166365384, 0.10304701160406694, -0.026839246395975... |
707.1772 | A note on the Hayman-Wu theorem | The Hayman-Wu theorem states that the preimage of a line or circle L under a
conformal mapping from the unit disc to a simply-connected domain U has total
Euclidean length bounded by an absolute constant. The best possible constant is
known to lie in the interval [pi^2, 4 pi), thanks to work of {\O}yma and Rohde.
Ear... | math.CV | the haymanwu theorem states that the preimage of a line or circle l under a conformal mapping from the unit disc to a simplyconnected domain u has total euclidean length bounded by an absolute constant the best possible constant is known to lie in the interval pi2 4 pi thanks to work of oyma and rohde earlier brown fli... | [['the', 'haymanwu', 'theorem', 'states', 'that', 'the', 'preimage', 'of', 'a', 'line', 'or', 'circle', 'l', 'under', 'a', 'conformal', 'mapping', 'from', 'the', 'unit', 'disc', 'to', 'a', 'simplyconnected', 'domain', 'u', 'has', 'total', 'euclidean', 'length', 'bounded', 'by', 'an', 'absolute', 'constant', 'the', 'bes... | [-0.16468520055980615, 0.12201798495909001, -0.018833744101789143, 7.876072065542928e-05, -0.07930711811917612, -0.1717090484076481, 0.06519599573807322, 0.34212792348518645, -0.2960279899852002, -0.22091325486025257, 0.09207786532896135, -0.29400453708643803, -0.08314254257673893, 0.18227241436193745, -0.0844551949471... |
707.1773 | Pyroelectric Effect Induced by the Built-in Field in the p-n Junction of
the Quantum Paraelectric PbTe: Experimental Study | We report here the first observation of a pyroelectric effect in a non-polar
semiconductor. This effect originates in the temperature dependent electric
dipole of the p-n junction. The junction was illuminated by a chopped CO2 laser
beam, and periodic and single-pulse pyroelectric signals were observed and
measured a... | cond-mat.other | we report here the first observation of a pyroelectric effect in a nonpolar semiconductor this effect originates in the temperature dependent electric dipole of the pn junction the junction was illuminated by a chopped co2 laser beam and periodic and singlepulse pyroelectric signals were observed and measured as a func... | [['we', 'report', 'here', 'the', 'first', 'observation', 'of', 'a', 'pyroelectric', 'effect', 'in', 'a', 'nonpolar', 'semiconductor', 'this', 'effect', 'originates', 'in', 'the', 'temperature', 'dependent', 'electric', 'dipole', 'of', 'the', 'pn', 'junction', 'the', 'junction', 'was', 'illuminated', 'by', 'a', 'chopped... | [-0.18542337658620633, 0.1644575912403045, -0.0418544888987646, -0.024170463485131553, -0.027414387291563407, -0.10159210874033826, 0.0758615461111601, 0.4180436331655953, -0.2458702515155732, -0.32279470579309777, 0.0025886375633590334, -0.29375443475034374, -0.07121878971888142, 0.21142372480532215, 0.027599969837215... |
707.1774 | The Poisson Kernel for Hardy Algebras | This note contributes to a circle of ideas that we have been developing
recently in which we view certain abstract operator algebras $H^{\infty}(E)$,
which we call Hardy algebras, and which are noncommutative generalizations of
classical $H^{\infty}$, as spaces of functions defined on their spaces of
representations.... | math.OA | this note contributes to a circle of ideas that we have been developing recently in which we view certain abstract operator algebras hinftye which we call hardy algebras and which are noncommutative generalizations of classical hinfty as spaces of functions defined on their spaces of representations we define a general... | [['this', 'note', 'contributes', 'to', 'a', 'circle', 'of', 'ideas', 'that', 'we', 'have', 'been', 'developing', 'recently', 'in', 'which', 'we', 'view', 'certain', 'abstract', 'operator', 'algebras', 'hinftye', 'which', 'we', 'call', 'hardy', 'algebras', 'and', 'which', 'are', 'noncommutative', 'generalizations', 'of'... | [-0.05602278963098643, 0.05549698011805369, -0.14128066241924822, 0.11883476613545266, -0.11627687028491161, -0.07445839259930899, -0.00100564080598751, 0.3727607357145195, -0.3254682699441385, -0.20378425643897394, 0.10486526951164296, -0.25716619090583753, -0.22581126842595323, 0.23422273926266376, -0.126474459199247... |
707.1775 | On the Rayleigh theorem for inflectional velocity instability of
inviscid flows | It is exactly proved that the classical Rayleigh Theorem on inflectional
velocity instability is wrong which states that the necessary condition for
instability of inviscid flow is the existence of an inflection point on the
velocity profile. It is shown that the disturbance amplified in 2D inviscid
flows is necessar... | physics.flu-dyn physics.class-ph physics.geo-ph | it is exactly proved that the classical rayleigh theorem on inflectional velocity instability is wrong which states that the necessary condition for instability of inviscid flow is the existence of an inflection point on the velocity profile it is shown that the disturbance amplified in 2d inviscid flows is necessarily... | [['it', 'is', 'exactly', 'proved', 'that', 'the', 'classical', 'rayleigh', 'theorem', 'on', 'inflectional', 'velocity', 'instability', 'is', 'wrong', 'which', 'states', 'that', 'the', 'necessary', 'condition', 'for', 'instability', 'of', 'inviscid', 'flow', 'is', 'the', 'existence', 'of', 'an', 'inflection', 'point', '... | [-0.22851456707847023, 0.16270407839548953, -0.1305559107080795, 0.06439033613220767, -0.0716222443477099, -0.10389881974714267, -0.05628955066691391, 0.2895765117651155, -0.30883861727319484, -0.17402326269075274, 0.11682454053567029, -0.21359675440417472, -0.11162778525071781, 0.18582771154293834, -0.0216905087080979... |
707.1776 | M{\o}ller Energy-Momentum Complex in General Relativity for Higher
Dimensional Universes | This submission has been withdrawn by arXiv administrators due to
inappropriate text reuse from external sources
| gr-qc | this submission has been withdrawn by arxiv administrators due to inappropriate text reuse from external sources | [['this', 'submission', 'has', 'been', 'withdrawn', 'by', 'arxiv', 'administrators', 'due', 'to', 'inappropriate', 'text', 'reuse', 'from', 'external', 'sources']] | [-0.090568175772205, -0.032664851227309555, -0.04400465509388596, -0.015228218551783357, -0.2861636411398649, -0.1730231347028166, 0.1099564551259391, 0.3669642357053817, -0.24552410130854696, -0.3927009613253176, 0.09520786831853911, -0.3657632351387292, -0.016878281836397946, -0.012412965414114296, -0.313948037917725... |
707.1777 | Atomistic Study of the Encapsulation of Diamondoids Inside Carbon
Nanotubes | The encapsulation of hydrogen-terminated nanosized diamond fragments (the
so-called diamondoids) into armchair single walled carbon nanotubes with
diameters in the range of 1.0 up to 2.2 nm has been investigated using
classical molecular dynamics simulations. Diameter dependent molecular ordered
phases were found for... | cond-mat.mtrl-sci | the encapsulation of hydrogenterminated nanosized diamond fragments the socalled diamondoids into armchair single walled carbon nanotubes with diameters in the range of 10 up to 22 nm has been investigated using classical molecular dynamics simulations diameter dependent molecular ordered phases were found for the enca... | [['the', 'encapsulation', 'of', 'hydrogenterminated', 'nanosized', 'diamond', 'fragments', 'the', 'socalled', 'diamondoids', 'into', 'armchair', 'single', 'walled', 'carbon', 'nanotubes', 'with', 'diameters', 'in', 'the', 'range', 'of', '10', 'up', 'to', '22', 'nm', 'has', 'been', 'investigated', 'using', 'classical', ... | [-0.10806174100373878, 0.19567958457392995, -0.005384896855388662, -0.009969104420181788, 0.00842637886588802, -0.1522417908623636, 0.031565048876859826, 0.49678089621359717, -0.22477148627042548, -0.335771047733278, 0.017281369372371385, -0.30594818807112245, -0.09886214550595708, 0.14213642708728547, 0.04663394273308... |
707.1778 | Angular Broadening of Intraday Variable AGN. II. Interstellar and
Intergalactic Scattering | We analyze a sample of 58 multi-wavelength, Very Long Baseline Array
observations of active galactic nuclei (AGN) to determine their scattering
properties. Approximately 75% of the sample consists of AGN that exhibit
centimeter-wavelength intraday variability (interstellar scintillation) while
the other 25% do not sh... | astro-ph | we analyze a sample of 58 multiwavelength very long baseline array observations of active galactic nuclei agn to determine their scattering properties approximately 75 of the sample consists of agn that exhibit centimeterwavelength intraday variability interstellar scintillation while the other 25 do not show intraday ... | [['we', 'analyze', 'a', 'sample', 'of', '58', 'multiwavelength', 'very', 'long', 'baseline', 'array', 'observations', 'of', 'active', 'galactic', 'nuclei', 'agn', 'to', 'determine', 'their', 'scattering', 'properties', 'approximately', '75', 'of', 'the', 'sample', 'consists', 'of', 'agn', 'that', 'exhibit', 'centimeter... | [-0.04469571867373297, 0.15508082381498264, -0.06544421599657989, 0.12257854214001701, -0.10277017848154747, -0.08053332554498112, 0.05841568705390196, 0.48614266445209464, -0.1714613175989282, -0.3403745868942704, 0.04214395691143222, -0.3379208137501914, 0.010536627948703057, 0.20379506697949307, -0.00273618841053820... |
707.1779 | Variational formulation of the motion of an ideal fluid on the basis of
gauge principle | On the basis of gauge principle in the field theory, a new variational
formulation is presented for flows of an ideal fluid. The fluid is defined
thermodynamically by mass density and entropy density, and its flow fields are
characterized by symmetries of translation and rotation. A structure of
rotation symmetry is ... | nlin.CD | on the basis of gauge principle in the field theory a new variational formulation is presented for flows of an ideal fluid the fluid is defined thermodynamically by mass density and entropy density and its flow fields are characterized by symmetries of translation and rotation a structure of rotation symmetry is equipp... | [['on', 'the', 'basis', 'of', 'gauge', 'principle', 'in', 'the', 'field', 'theory', 'a', 'new', 'variational', 'formulation', 'is', 'presented', 'for', 'flows', 'of', 'an', 'ideal', 'fluid', 'the', 'fluid', 'is', 'defined', 'thermodynamically', 'by', 'mass', 'density', 'and', 'entropy', 'density', 'and', 'its', 'flow',... | [-0.19363647988052696, 0.14786199477501882, -0.11133329586350713, 0.03345913651410019, -0.0734225156912366, -0.07237176085961447, -0.043959574349058644, 0.29546068819111276, -0.30081747762387856, -0.2703259229023095, 0.048230987180682736, -0.2374092759029276, -0.10959479646173831, 0.14187987600640534, -0.03700371748692... |
707.178 | A classification of entanglement in three-qubit systems | We present a classification of three-qubit states based in their three-qubit
and reduced two-qubit entanglements. For pure states these criteria can be
easily implemented, and the different types can be related with sets of
equivalence classes under Local Unitary operations. For mixed states
characterization of full ... | quant-ph | we present a classification of threequbit states based in their threequbit and reduced twoqubit entanglements for pure states these criteria can be easily implemented and the different types can be related with sets of equivalence classes under local unitary operations for mixed states characterization of full triparti... | [['we', 'present', 'a', 'classification', 'of', 'threequbit', 'states', 'based', 'in', 'their', 'threequbit', 'and', 'reduced', 'twoqubit', 'entanglements', 'for', 'pure', 'states', 'these', 'criteria', 'can', 'be', 'easily', 'implemented', 'and', 'the', 'different', 'types', 'can', 'be', 'related', 'with', 'sets', 'of... | [-0.09847793719716004, 0.20353196285756642, -0.07775623675008289, 0.05954727861213452, 0.020125119595742615, -0.23234324594654265, 0.04063631938083372, 0.38534110595212606, -0.25209739956943716, -0.26258767682478806, 0.1333753938107278, -0.17742921478405108, -0.09841632888056949, 0.2267173739974616, -0.0885318825708427... |
707.1781 | Calculation of the metric in the Hilbert space of a PT-symmetric model
via the spectral theorem | In a previous paper (arXiv:math-ph/0604055) we introduced a very simple
PT-symmetric non-Hermitian Hamiltonian with real spectrum and derived a closed
formula for the metric operator relating the problem to a Hermitian one. In
this note we propose an alternative formula for the metric operator, which we
believe is mo... | math-ph math.MP quant-ph | in a previous paper arxivmathph0604055 we introduced a very simple ptsymmetric nonhermitian hamiltonian with real spectrum and derived a closed formula for the metric operator relating the problem to a hermitian one in this note we propose an alternative formula for the metric operator which we believe is more elegant ... | [['in', 'a', 'previous', 'paper', 'arxivmathph0604055', 'we', 'introduced', 'a', 'very', 'simple', 'ptsymmetric', 'nonhermitian', 'hamiltonian', 'with', 'real', 'spectrum', 'and', 'derived', 'a', 'closed', 'formula', 'for', 'the', 'metric', 'operator', 'relating', 'the', 'problem', 'to', 'a', 'hermitian', 'one', 'in', ... | [-0.10944714204389092, 0.04871727745802212, -0.1494112672820075, 0.087672937610378, -0.13128343332010284, -0.17228485347243816, 0.02787237271446454, 0.33361559468385293, -0.22393045051355068, -0.2211578894814808, 0.06848385788768224, -0.24424865913309463, -0.24292381977254193, 0.21893501083672762, -0.10032872190979654,... |
707.1782 | Magnetic reconnection at the termination shock in a striped pulsar wind | Most of the rotational luminosity of a pulsar is carried away by a
relativistic magnetised wind in which the matter energy flux is negligible
compared to the Poynting flux. Near the equatorial plane of an obliquely
rotating pulsar magnetosphere, the magnetic field reverses polarity with the
pulsar period, forming a w... | astro-ph | most of the rotational luminosity of a pulsar is carried away by a relativistic magnetised wind in which the matter energy flux is negligible compared to the poynting flux near the equatorial plane of an obliquely rotating pulsar magnetosphere the magnetic field reverses polarity with the pulsar period forming a wind w... | [['most', 'of', 'the', 'rotational', 'luminosity', 'of', 'a', 'pulsar', 'is', 'carried', 'away', 'by', 'a', 'relativistic', 'magnetised', 'wind', 'in', 'which', 'the', 'matter', 'energy', 'flux', 'is', 'negligible', 'compared', 'to', 'the', 'poynting', 'flux', 'near', 'the', 'equatorial', 'plane', 'of', 'an', 'obliquel... | [-0.1912771288341689, 0.18614561133014912, -0.02035034356132439, 0.10300304983024723, -0.10299815375299093, -0.08214584085638228, -0.015609538724569116, 0.38684988372678897, -0.25177555312730315, -0.3061463241781859, 0.029796266776297098, -0.2130471203932245, 0.005166924979031375, 0.24669708286974923, 0.057686386467183... |
707.1783 | A Photometrically Detected Forming Cluster of Galaxies at Redshift 1.6
in the GOODS Field | We report the discovery of a localized overdensity at z~1.6 in the
GOODS-South Field, presumably a poor cluster in the process of formation. The
three-dimensional galaxy density has been estimated on the basis of well
calibrated photometric redshifts from the multiband photometric GOODS-MUSIC
catalog using the (2+1)D... | astro-ph | we report the discovery of a localized overdensity at z16 in the goodssouth field presumably a poor cluster in the process of formation the threedimensional galaxy density has been estimated on the basis of well calibrated photometric redshifts from the multiband photometric goodsmusic catalog using the 21d technique t... | [['we', 'report', 'the', 'discovery', 'of', 'a', 'localized', 'overdensity', 'at', 'z16', 'in', 'the', 'goodssouth', 'field', 'presumably', 'a', 'poor', 'cluster', 'in', 'the', 'process', 'of', 'formation', 'the', 'threedimensional', 'galaxy', 'density', 'has', 'been', 'estimated', 'on', 'the', 'basis', 'of', 'well', '... | [-0.06848416503370655, 0.09574393399725523, -0.08475097401903688, 0.09233245942634354, -0.05903315052405973, -0.011645016439036805, 0.06280471449149032, 0.439302877697628, -0.10704397542444481, -0.3809574829329821, 0.0675681791094989, -0.31182285121493886, 0.015375772467285225, 0.18277116580231284, -0.0055582379758231,... |
707.1784 | Recent developments in heavy flavour production | We review one-particle inclusive production of heavy-flavoured hadrons in a
framework which resums the large collinear logarithms through the evolution of
the FFs and PDFs and retains the full dependence on the heavy-quark mass
without additional theoretical assumptions. We focus on presenting results for
the inclusi... | hep-ph | we review oneparticle inclusive production of heavyflavoured hadrons in a framework which resums the large collinear logarithms through the evolution of the ffs and pdfs and retains the full dependence on the heavyquark mass without additional theoretical assumptions we focus on presenting results for the inclusive cro... | [['we', 'review', 'oneparticle', 'inclusive', 'production', 'of', 'heavyflavoured', 'hadrons', 'in', 'a', 'framework', 'which', 'resums', 'the', 'large', 'collinear', 'logarithms', 'through', 'the', 'evolution', 'of', 'the', 'ffs', 'and', 'pdfs', 'and', 'retains', 'the', 'full', 'dependence', 'on', 'the', 'heavyquark',... | [0.00021689095430903963, 0.13724673041283633, -0.14469996821417502, 0.11872120089288048, -0.03329161757772619, -0.032946575859872006, 0.016377587699227862, 0.3081672488137929, -0.14754245179996947, -0.22611454777381937, -0.041904792978635266, -0.4277747722455498, 0.07784351679223656, 0.12785154863288908, 0.105623922070... |
707.1785 | Instabilities for supercritical Schr\"odinger equations in analytic
manifolds | In this paper we consider supercritical nonlinear Schr\"odinger equations in
an analytic Riemannian manifold $(M^d,g)$, where the metric $g$ is analytic.
Using an analytic WKB method, we are able to construct an Ansatz for the
semiclassical equation for times independent of the small parameter. These
approximate solu... | math.AP math-ph math.MP | in this paper we consider supercritical nonlinear schrodinger equations in an analytic riemannian manifold mdg where the metric g is analytic using an analytic wkb method we are able to construct an ansatz for the semiclassical equation for times independent of the small parameter these approximate solutions will help ... | [['in', 'this', 'paper', 'we', 'consider', 'supercritical', 'nonlinear', 'schrodinger', 'equations', 'in', 'an', 'analytic', 'riemannian', 'manifold', 'mdg', 'where', 'the', 'metric', 'g', 'is', 'analytic', 'using', 'an', 'analytic', 'wkb', 'method', 'we', 'are', 'able', 'to', 'construct', 'an', 'ansatz', 'for', 'the',... | [-0.13632319341903845, 0.051172643229763615, -0.0785130837527839, 0.11068972491193563, -0.10309706421838583, -0.06372828898020089, -0.06044439974357374, 0.35241149037488195, -0.25731762974081857, -0.2185511509887874, 0.10294244768661692, -0.28242541986860725, -0.14457023401107444, 0.18860188511960013, -0.07821894647847... |
707.1786 | A new approach to the giant component problem | We study the largest component of a random (multi)graph on n vertices with a
given degree sequence. We let n tend to infinity. Then, under some regularity
conditions on the degree sequences, we give conditions on the asymptotic shape
of the degree sequence that imply that with high probability all the components
are ... | math.CO math.PR | we study the largest component of a random multigraph on n vertices with a given degree sequence we let n tend to infinity then under some regularity conditions on the degree sequences we give conditions on the asymptotic shape of the degree sequence that imply that with high probability all the components are small an... | [['we', 'study', 'the', 'largest', 'component', 'of', 'a', 'random', 'multigraph', 'on', 'n', 'vertices', 'with', 'a', 'given', 'degree', 'sequence', 'we', 'let', 'n', 'tend', 'to', 'infinity', 'then', 'under', 'some', 'regularity', 'conditions', 'on', 'the', 'degree', 'sequences', 'we', 'give', 'conditions', 'on', 'th... | [-0.13523691365403603, 0.1421966799309082, -0.09125368414503156, 0.0068941640484174995, -0.05113854874913214, -0.11948895703606081, 0.06313614506048687, 0.35884918347001077, -0.2288441934989709, -0.27840376315977083, 0.11381803508054211, -0.27722177752716975, -0.1384970908391882, 0.16701451994930253, -0.084713453973403... |
707.1787 | Canonical connections on paracontact manifolds | The canonical paracontact connection is defined and it is shown that its
torsion is the obstruction the paracontact manifold to be paraSasakian. A
$\mathcal{D}$-homothetic transformation is determined as a special gauge
transformation. The $\eta$-Einstein manifold are defined, it is prove that
their scalar curvature ... | math.DG | the canonical paracontact connection is defined and it is shown that its torsion is the obstruction the paracontact manifold to be parasasakian a mathcaldhomothetic transformation is determined as a special gauge transformation the etaeinstein manifold are defined it is prove that their scalar curvature is a constant a... | [['the', 'canonical', 'paracontact', 'connection', 'is', 'defined', 'and', 'it', 'is', 'shown', 'that', 'its', 'torsion', 'is', 'the', 'obstruction', 'the', 'paracontact', 'manifold', 'to', 'be', 'parasasakian', 'a', 'mathcaldhomothetic', 'transformation', 'is', 'determined', 'as', 'a', 'special', 'gauge', 'transformat... | [-0.25958361675125513, 0.12064816080307467, -0.10524327444391719, 0.09268590507249777, -0.190796128492086, -0.18285538909885174, -0.16279538167425647, 0.4279468218401934, -0.2953753089845682, -0.18670434763099855, 0.10892186290220707, -0.25620641575705333, -0.2821295845787972, 0.10555179143109573, -0.08122433407697827,... |
707.1788 | Searching for the Critical Point of QCD: Theoretical Benchmark
Calculations | We present a comprehensive study of event-by-event multiplicity fluctuations
in nucleon-nucleon and nucleus-nucleus interactions from AGS/FAIR to RHIC
energies within the UrQMD transport approach. The scaled variances of negative,
positive, and all charged hadrons are analysed. The scaled variance in central
Pb+Pb co... | nucl-th | we present a comprehensive study of eventbyevent multiplicity fluctuations in nucleonnucleon and nucleusnucleus interactions from agsfair to rhic energies within the urqmd transport approach the scaled variances of negative positive and all charged hadrons are analysed the scaled variance in central pbpb collisions inc... | [['we', 'present', 'a', 'comprehensive', 'study', 'of', 'eventbyevent', 'multiplicity', 'fluctuations', 'in', 'nucleonnucleon', 'and', 'nucleusnucleus', 'interactions', 'from', 'agsfair', 'to', 'rhic', 'energies', 'within', 'the', 'urqmd', 'transport', 'approach', 'the', 'scaled', 'variances', 'of', 'negative', 'positi... | [-0.08635025314753875, 0.18337023650296033, -0.20560609558713622, 0.18745115612167865, 0.03348288998473436, -0.07506312132813037, -0.0579751790582668, 0.34199929631082343, -0.16982540071941912, -0.29375423399731515, -0.08011652101995423, -0.39006959507241845, 0.07544737357180566, 0.1256162715679966, 0.05232962006470188... |
707.1789 | ChPT Progress on Non-Leptonic and Radiative Kaon Decays | I discuss recent developments on non-leptonic and radiative kaon decays
mainly related to direct CP-violation within the combined ChPT and 1/N_c
expansion approaches. In particular, I review the status of K -> pi pi,
epsilon_K', direct CP-violating K+ -> 3 pi Dalitz plot slope g and decay rate
asymmetries, and the St... | hep-ph hep-ex hep-lat | i discuss recent developments on nonleptonic and radiative kaon decays mainly related to direct cpviolation within the combined chpt and 1n_c expansion approaches in particular i review the status of k pi pi epsilon_k direct cpviolating k 3 pi dalitz plot slope g and decay rate asymmetries and the standard model predic... | [['i', 'discuss', 'recent', 'developments', 'on', 'nonleptonic', 'and', 'radiative', 'kaon', 'decays', 'mainly', 'related', 'to', 'direct', 'cpviolation', 'within', 'the', 'combined', 'chpt', 'and', '1n_c', 'expansion', 'approaches', 'in', 'particular', 'i', 'review', 'the', 'status', 'of', 'k', 'pi', 'pi', 'epsilon_k'... | [-0.10128911037259457, 0.2232700369010369, -0.04435347251414338, 0.09955418165446374, -0.10425429570635683, -0.16151467086583898, 0.16463370078954062, 0.25049142199650143, -0.22535289624673233, -0.162115290695638, -0.07973924011866186, -0.4061444438503761, -0.01571570323747501, 0.08966746633431237, 0.11454780191885666,... |
707.179 | A note on the radial solutions for the supercritical Henon equation | We prove the existence of a positive radial solution for the H\'enon equation
with arbitrary growth. The solution is found by means of a shooting method and
turns out to be an increasing function of the radial variable. Some numerical
experiments suggest the existence of many positive oscillating solutions.
| math.AP | we prove the existence of a positive radial solution for the henon equation with arbitrary growth the solution is found by means of a shooting method and turns out to be an increasing function of the radial variable some numerical experiments suggest the existence of many positive oscillating solutions | [['we', 'prove', 'the', 'existence', 'of', 'a', 'positive', 'radial', 'solution', 'for', 'the', 'henon', 'equation', 'with', 'arbitrary', 'growth', 'the', 'solution', 'is', 'found', 'by', 'means', 'of', 'a', 'shooting', 'method', 'and', 'turns', 'out', 'to', 'be', 'an', 'increasing', 'function', 'of', 'the', 'radial', ... | [-0.1629116112082408, 0.058536118801923144, -0.14152639043726484, 0.028935042963059127, -0.07373718810932976, -0.13130177392111142, -0.0016148258760875585, 0.282806397463214, -0.2853868978896311, -0.2439658476838044, 0.14397017474343277, -0.31828779240652005, -0.1608890431020789, 0.24205527435608057, 0.0342411216804567... |
707.1791 | Bistability in superconducting rings containing an inhomogeneous
Josephson junction | We investigate the magnetic response of a superconducting Nb ring containing
a ferromagnetic PdNi Josephson junction and a tunnel junction in parallel. A
doubling of the switching frequency is observed within certain intervals of the
external magnetic field. Assuming sinusoidal current-phase relations of both
junctio... | cond-mat.mes-hall | we investigate the magnetic response of a superconducting nb ring containing a ferromagnetic pdni josephson junction and a tunnel junction in parallel a doubling of the switching frequency is observed within certain intervals of the external magnetic field assuming sinusoidal currentphase relations of both junctions ou... | [['we', 'investigate', 'the', 'magnetic', 'response', 'of', 'a', 'superconducting', 'nb', 'ring', 'containing', 'a', 'ferromagnetic', 'pdni', 'josephson', 'junction', 'and', 'a', 'tunnel', 'junction', 'in', 'parallel', 'a', 'doubling', 'of', 'the', 'switching', 'frequency', 'is', 'observed', 'within', 'certain', 'inter... | [-0.3481968696046945, 0.17505350007432635, 0.0051229586723544026, 0.02715700518582826, -0.02170057576807702, -0.12426742504897487, 0.07808576267258183, 0.397519306158242, -0.22986230893951395, -0.3067570058628917, -0.028462782977958737, -0.24019920119367863, -0.07359387215388857, 0.21710111006699584, 0.0522721716374887... |
707.1792 | Evolution of low-mass star and brown dwarf eclipsing binaries | We examine the evolution of low-mass star and brown dwarf eclipsing binaries.
These objects are rapid rotators and are believed to shelter large magnetic
fields. We suggest that reduced convective efficiency, due to fast rotation and
large field strengths, and/or to magnetic spot coverage of the radiating
surface sig... | astro-ph | we examine the evolution of lowmass star and brown dwarf eclipsing binaries these objects are rapid rotators and are believed to shelter large magnetic fields we suggest that reduced convective efficiency due to fast rotation and large field strengths andor to magnetic spot coverage of the radiating surface significant... | [['we', 'examine', 'the', 'evolution', 'of', 'lowmass', 'star', 'and', 'brown', 'dwarf', 'eclipsing', 'binaries', 'these', 'objects', 'are', 'rapid', 'rotators', 'and', 'are', 'believed', 'to', 'shelter', 'large', 'magnetic', 'fields', 'we', 'suggest', 'that', 'reduced', 'convective', 'efficiency', 'due', 'to', 'fast',... | [-0.11312138338836682, 0.2134155839954437, -0.03812524873405845, 0.12557344424075004, -0.10473340264088804, -0.07814033698252958, 0.08436774408839869, 0.37151800836389415, -0.1743229887250698, -0.38943126071432627, 0.05185912484938109, -0.26491737329034193, -0.08066807498420016, 0.2327735457672841, -0.05818427426063202... |
707.1793 | Near-UV Merger Signatures in Early-Type Galaxies | Hierarchical assembly of early-type galaxies (Es and S0s) over an extended
period of time will result in mixed-generation stellar populations. Here we
look for signatures of composite populations in broad-band, near-ultraviolet
(2500-3400 A), high-resolution HST imaging of the cores of 12 bright early-type
galaxies w... | astro-ph | hierarchical assembly of earlytype galaxies es and s0s over an extended period of time will result in mixedgeneration stellar populations here we look for signatures of composite populations in broadband nearultraviolet 25003400 a highresolution hst imaging of the cores of 12 bright earlytype galaxies without obvious d... | [['hierarchical', 'assembly', 'of', 'earlytype', 'galaxies', 'es', 'and', 's0s', 'over', 'an', 'extended', 'period', 'of', 'time', 'will', 'result', 'in', 'mixedgeneration', 'stellar', 'populations', 'here', 'we', 'look', 'for', 'signatures', 'of', 'composite', 'populations', 'in', 'broadband', 'nearultraviolet', '2500... | [-0.04565102624167737, 0.1548995623354322, -0.09170433231874515, 0.12693820906141282, -0.0645470357058864, -0.08245906578867059, 0.026655192543311338, 0.4994812600314617, -0.09615291890835291, -0.39116080484205956, 0.039164799938321504, -0.2686370008085903, 0.0002500788774341345, 0.18322644280514827, -0.048594766149395... |
707.1794 | Scaling study of the pion electroproduction cross sections and the pion
form factor | The $^{1}$H($e,e^\prime \pi^+$)n cross section was measured for a range of
four-momentum transfer up to $Q^2$=3.91 GeV$^2$ at values of the invariant
mass, $W$, above the resonance region. The $Q^2$-dependence of the longitudinal
component is consistent with the $Q^2$-scaling prediction for hard exclusive
processes. ... | nucl-ex | the 1heeprime pin cross section was measured for a range of fourmomentum transfer up to q2391 gev2 at values of the invariant mass w above the resonance region the q2dependence of the longitudinal component is consistent with the q2scaling prediction for hard exclusive processes this suggests that perturbative qcd conc... | [['the', '1heeprime', 'pin', 'cross', 'section', 'was', 'measured', 'for', 'a', 'range', 'of', 'fourmomentum', 'transfer', 'up', 'to', 'q2391', 'gev2', 'at', 'values', 'of', 'the', 'invariant', 'mass', 'w', 'above', 'the', 'resonance', 'region', 'the', 'q2dependence', 'of', 'the', 'longitudinal', 'component', 'is', 'co... | [-0.051312140712403864, 0.2073593888164378, -0.07519454260052431, 0.12939052241347213, -0.029181859882474685, -0.06703694549269311, 0.03978387810437396, 0.37772208950159575, -0.19121790754765566, -0.24823168882786636, -0.03656277602358657, -0.3392487698243839, 0.05123679184050548, 0.1663876136575853, 0.0552425804973861... |
707.1795 | Stochastic analysis and simulation of spin star systems | We discuss two methods of an exact stochastic representation of the
non-Markovian quantum dynamics of open systems. The first method employs a pair
of stochastic product vectors in the total system's state space, while the
second method uses a pair of state vectors in the open system's state space and
a random operat... | quant-ph | we discuss two methods of an exact stochastic representation of the nonmarkovian quantum dynamics of open systems the first method employs a pair of stochastic product vectors in the total systems state space while the second method uses a pair of state vectors in the open systems state space and a random operator acti... | [['we', 'discuss', 'two', 'methods', 'of', 'an', 'exact', 'stochastic', 'representation', 'of', 'the', 'nonmarkovian', 'quantum', 'dynamics', 'of', 'open', 'systems', 'the', 'first', 'method', 'employs', 'a', 'pair', 'of', 'stochastic', 'product', 'vectors', 'in', 'the', 'total', 'systems', 'state', 'space', 'while', '... | [-0.14393880250001395, 0.08449272376989635, -0.07743867084521938, 0.052685184213677766, 0.0074995954314039815, -0.08440194587068012, 0.034631690983143115, 0.32203280674466106, -0.2693138620842041, -0.24814674623862462, 0.0926689380891966, -0.2875838462953214, -0.10789340855898681, 0.18344445973289786, 0.030952539087997... |
707.1796 | Donor binding energy and thermally activated persistent
photoconductivity in high mobility (001) AlAs quantum wells | A doping series of AlAs (001) quantum wells with Si delta-modulation doping
on both sides reveals different dark and post-illumination saturation
densities, as well as temperature dependent photoconductivity. The lower dark
two-dimensional electron density saturation is explained assuming deep binding
energy of Delta... | cond-mat.mes-hall | a doping series of alas 001 quantum wells with si deltamodulation doping on both sides reveals different dark and postillumination saturation densities as well as temperature dependent photoconductivity the lower dark twodimensional electron density saturation is explained assuming deep binding energy of delta_dk 652 m... | [['a', 'doping', 'series', 'of', 'alas', '001', 'quantum', 'wells', 'with', 'si', 'deltamodulation', 'doping', 'on', 'both', 'sides', 'reveals', 'different', 'dark', 'and', 'postillumination', 'saturation', 'densities', 'as', 'well', 'as', 'temperature', 'dependent', 'photoconductivity', 'the', 'lower', 'dark', 'twodim... | [-0.10954067833557889, 0.2388488871997202, -0.04222653179869547, 0.08863638640652605, 0.022980949993355322, -0.24047928334694807, 0.07954426176057985, 0.42503478279808066, -0.19646010763820385, -0.42329400194460876, -0.04019766173627391, -0.3181426040623542, 0.007246690748545986, 0.1567594803700858, 0.00976247601415757... |
707.1797 | Possible Measurable Effects of Dark Energy in Rotating Superconductors | We discuss recent laboratory experiments with rotating superconductors and
show that three so far unexplained experimentally observed effects (anomalous
acceleration signals, anomalous gyroscope signals, Cooper pair mass excess) can
be physically explained in terms of a possible interaction of dark energy with
Cooper... | gr-qc astro-ph cond-mat.supr-con hep-th | we discuss recent laboratory experiments with rotating superconductors and show that three so far unexplained experimentally observed effects anomalous acceleration signals anomalous gyroscope signals cooper pair mass excess can be physically explained in terms of a possible interaction of dark energy with cooper pairs... | [['we', 'discuss', 'recent', 'laboratory', 'experiments', 'with', 'rotating', 'superconductors', 'and', 'show', 'that', 'three', 'so', 'far', 'unexplained', 'experimentally', 'observed', 'effects', 'anomalous', 'acceleration', 'signals', 'anomalous', 'gyroscope', 'signals', 'cooper', 'pair', 'mass', 'excess', 'can', 'b... | [-0.16467344906413928, 0.2408420777441386, -0.056636598043362886, 0.1171266201289494, -0.08344253162880812, -0.14046885937675732, 0.028454564059810603, 0.33765330238213, -0.18926245254217922, -0.36056197258671197, -0.04137033982175019, -0.2865259190405007, -0.10315069446668905, 0.19822609227369814, 0.008491772370796432... |
707.1798 | Density-PDFs and Lagrangian Statistics of highly compressible Turbulence | We report on probability-density-functions (PDF) of the mass density in
numerical simulations of highly compressible hydrodynamic flows and the
corresponding structure formation of Lagrangian particles advected by the
flows. Numerical simulations were performed with $512^3$ collocation points and
2 million tracer par... | physics.flu-dyn | we report on probabilitydensityfunctions pdf of the mass density in numerical simulations of highly compressible hydrodynamic flows and the corresponding structure formation of lagrangian particles advected by the flows numerical simulations were performed with 5123 collocation points and 2 million tracer particles int... | [['we', 'report', 'on', 'probabilitydensityfunctions', 'pdf', 'of', 'the', 'mass', 'density', 'in', 'numerical', 'simulations', 'of', 'highly', 'compressible', 'hydrodynamic', 'flows', 'and', 'the', 'corresponding', 'structure', 'formation', 'of', 'lagrangian', 'particles', 'advected', 'by', 'the', 'flows', 'numerical'... | [-0.17455132648880992, 0.13975768689831186, -0.13199553090546812, 0.03474655432094421, 0.08676892188045063, -0.028585978519237998, -0.03468621564762933, 0.3352857076363372, -0.20764304313010404, -0.35596472424055847, 0.0475529337534681, -0.31413195739899363, -0.06639239064284734, 0.12485339411401324, 0.0868583964050880... |
707.1799 | Open string with a background B-field as the first order mechanics,
noncommutativity and soldering formalism | To study noncommutativity properties of the open string with constant B-field
we construct a mechanical action which reproduces classical dynamics of the
string sector under consideration. It allows one to apply the Dirac
quantization procedure for constrained systems in a direct and unambiguous way.
The mechanical a... | hep-th | to study noncommutativity properties of the open string with constant bfield we construct a mechanical action which reproduces classical dynamics of the string sector under consideration it allows one to apply the dirac quantization procedure for constrained systems in a direct and unambiguous way the mechanical action... | [['to', 'study', 'noncommutativity', 'properties', 'of', 'the', 'open', 'string', 'with', 'constant', 'bfield', 'we', 'construct', 'a', 'mechanical', 'action', 'which', 'reproduces', 'classical', 'dynamics', 'of', 'the', 'string', 'sector', 'under', 'consideration', 'it', 'allows', 'one', 'to', 'apply', 'the', 'dirac',... | [-0.15989024822797487, 0.12966090515134976, -0.13805763162188717, 0.09237871865905192, -0.11175211684705762, -0.13550827003011554, 0.052484462098158026, 0.31354521427079796, -0.268622810903985, -0.29497818392701447, 0.06076978566805385, -0.22027565329023804, -0.17682783386984527, 0.14747077430441202, -0.073015133587208... |
707.18 | On the elastic moduli of three-dimensional assemblies of spheres:
characterization and modeling of fluctuations in the particle displacement
and rotation | The elastic moduli of four numerical random isotropic packings of Hertzian
spheres are studied. The four samples are assembled with different preparation
procedures, two of which aim to reproduce experimental compaction by vibration
and lubrication. The mechanical properties of the samples are found to change
with th... | cond-mat.mtrl-sci cond-mat.dis-nn cond-mat.stat-mech | the elastic moduli of four numerical random isotropic packings of hertzian spheres are studied the four samples are assembled with different preparation procedures two of which aim to reproduce experimental compaction by vibration and lubrication the mechanical properties of the samples are found to change with the pre... | [['the', 'elastic', 'moduli', 'of', 'four', 'numerical', 'random', 'isotropic', 'packings', 'of', 'hertzian', 'spheres', 'are', 'studied', 'the', 'four', 'samples', 'are', 'assembled', 'with', 'different', 'preparation', 'procedures', 'two', 'of', 'which', 'aim', 'to', 'reproduce', 'experimental', 'compaction', 'by', '... | [-0.13422162263804197, 0.1836338606020085, -0.08967859592195211, 0.037847994370814646, -0.01613193538788098, -0.08625400016984462, -0.0030169353964563193, 0.386990388317587, -0.2781420407980431, -0.3215701683927581, 0.08562843512722279, -0.29783813470670617, -0.11756185357908598, 0.17315827729716257, -0.002758270693615... |
707.1801 | Equations for Chow and Hilbert Quotients | We give explicit equations for the Chow and Hilbert quotients of a projective
scheme X by the action of an algebraic torus T in an auxiliary toric variety.
As a consequence we provide GIT descriptions of these canonical quotients, and
obtain other GIT quotients of X by variation of GIT quotient. We apply these
result... | math.AG | we give explicit equations for the chow and hilbert quotients of a projective scheme x by the action of an algebraic torus t in an auxiliary toric variety as a consequence we provide git descriptions of these canonical quotients and obtain other git quotients of x by variation of git quotient we apply these results to ... | [['we', 'give', 'explicit', 'equations', 'for', 'the', 'chow', 'and', 'hilbert', 'quotients', 'of', 'a', 'projective', 'scheme', 'x', 'by', 'the', 'action', 'of', 'an', 'algebraic', 'torus', 't', 'in', 'an', 'auxiliary', 'toric', 'variety', 'as', 'a', 'consequence', 'we', 'provide', 'git', 'descriptions', 'of', 'these'... | [-0.20632917673131565, 0.00951787967121309, -0.15974594297370426, 0.08402825579231168, -0.0796040138574662, -0.11662210209042202, -0.0025460098490670876, 0.3033940470604985, -0.38656063189293133, -0.16869583531041388, 0.12622181501923657, -0.18890930232764394, -0.15421380483211927, 0.2708353432309296, -0.22138149033725... |
707.1802 | On the solutions of the dKP equation: nonlinear Riemann Hilbert problem,
longtime behaviour, implicit solutions and wave breaking | We make use of the nonlinear Riemann Hilbert problem of the dispersionless
Kadomtsev Petviashvili equation, i) to construct the longtime behaviour of the
solutions of its Cauchy problem; ii) to characterize a class of implicit
solutions; iii) to elucidate the spectral mechanism causing the gradient
catastrophe of loc... | nlin.SI | we make use of the nonlinear riemann hilbert problem of the dispersionless kadomtsev petviashvili equation i to construct the longtime behaviour of the solutions of its cauchy problem ii to characterize a class of implicit solutions iii to elucidate the spectral mechanism causing the gradient catastrophe of localized s... | [['we', 'make', 'use', 'of', 'the', 'nonlinear', 'riemann', 'hilbert', 'problem', 'of', 'the', 'dispersionless', 'kadomtsev', 'petviashvili', 'equation', 'i', 'to', 'construct', 'the', 'longtime', 'behaviour', 'of', 'the', 'solutions', 'of', 'its', 'cauchy', 'problem', 'ii', 'to', 'characterize', 'a', 'class', 'of', 'i... | [-0.125799351234243, 0.035465908827697575, -0.09113597447250152, 0.12323326968489158, -0.08256308960192131, -0.12928153190648917, 0.007717266283703573, 0.2720733093323581, -0.3582155827545758, -0.21485861102965745, 0.15167975487279226, -0.2817591775886037, -0.15104724598738054, 0.14115112403294805, -0.00940205993582353... |
707.1803 | Local dielectric spectroscopy of near-surface glassy polymer dynamics | A non-contact scanning-probe-microscopy method was used to probe local
near-surface dielectric susceptibility and dielectric relaxation in
poly-vinyl-acetate (PVAc) near the glass transition. Dielectric spectra were
measured from 10-4 Hz to 102 Hz as a function of temperature. The measurements
probed a 20 nm thick la... | cond-mat.soft cond-mat.dis-nn | a noncontact scanningprobemicroscopy method was used to probe local nearsurface dielectric susceptibility and dielectric relaxation in polyvinylacetate pvac near the glass transition dielectric spectra were measured from 104 hz to 102 hz as a function of temperature the measurements probed a 20 nm thick layer below the... | [['a', 'noncontact', 'scanningprobemicroscopy', 'method', 'was', 'used', 'to', 'probe', 'local', 'nearsurface', 'dielectric', 'susceptibility', 'and', 'dielectric', 'relaxation', 'in', 'polyvinylacetate', 'pvac', 'near', 'the', 'glass', 'transition', 'dielectric', 'spectra', 'were', 'measured', 'from', '104', 'hz', 'to... | [-0.08754939280603964, 0.21085224286221044, -0.027524709432702705, -0.04317966772761849, 0.01871948808518037, -0.13639820887966408, 0.0596779549275957, 0.39667709905308546, -0.189503497981764, -0.32682229931821527, 0.04594363030118234, -0.32469554441337733, -0.050165025445335, 0.18383349934304805, 0.025292053032599238,... |
707.1804 | Properties of high-T$_C$ copper oxides from the nearly-free electron
model | The generic band structure of high-T$_C$ copper oxides is simulated by the
nearly free-electron model (NFE) in two dimensions (2-D) with parameters from
band calculations. Interaction between phonons and spin waves will cause
potential modulations and pseudogaps, and the strength of the modulations, the
wave lengths ... | cond-mat.supr-con cond-mat.mtrl-sci | the generic band structure of hight_c copper oxides is simulated by the nearly freeelectron model nfe in two dimensions 2d with parameters from band calculations interaction between phonons and spin waves will cause potential modulations and pseudogaps and the strength of the modulations the wave lengths and the doping... | [['the', 'generic', 'band', 'structure', 'of', 'hight_c', 'copper', 'oxides', 'is', 'simulated', 'by', 'the', 'nearly', 'freeelectron', 'model', 'nfe', 'in', 'two', 'dimensions', '2d', 'with', 'parameters', 'from', 'band', 'calculations', 'interaction', 'between', 'phonons', 'and', 'spin', 'waves', 'will', 'cause', 'po... | [-0.20994028123630876, 0.24051543281295862, 0.013676559627484316, 0.07274477951624699, -0.005246324472707407, -0.1662917554100183, 0.08695496720443854, 0.3927668543671654, -0.2665824970421475, -0.2757288956811957, -0.026229765048068572, -0.3671791348820445, -0.1349156973027121, 0.1900817093000501, 0.07470511346680765, ... |
707.1805 | Diffusion and transfer of entanglement in an array of inductively
coupled flux qubits | A theoretical scheme to generate multipartite entangled states in a Josephson
planar-designed architecture is reported. This scheme improves the one
published in [Phys. Rev. B 74, 104503 (2006)] since it speeds up the generation
of W entangled states in an MxN array of inductively coupled Josephson flux
qubits by red... | cond-mat.supr-con cond-mat.other quant-ph | a theoretical scheme to generate multipartite entangled states in a josephson planardesigned architecture is reported this scheme improves the one published in phys rev b 74 104503 2006 since it speeds up the generation of w entangled states in an mxn array of inductively coupled josephson flux qubits by reducing the n... | [['a', 'theoretical', 'scheme', 'to', 'generate', 'multipartite', 'entangled', 'states', 'in', 'a', 'josephson', 'planardesigned', 'architecture', 'is', 'reported', 'this', 'scheme', 'improves', 'the', 'one', 'published', 'in', 'phys', 'rev', 'b', '74', '104503', '2006', 'since', 'it', 'speeds', 'up', 'the', 'generatio... | [-0.14443295246550208, 0.17876552281499292, 0.009947692497155151, -0.06832873124497112, -9.724825016550116e-05, -0.21292181782474792, 0.10278378212761537, 0.3594771687042069, -0.20682607231995193, -0.32785215186005506, -0.019598166323015215, -0.26175410058223514, -0.05930742182661905, 0.20352340613592518, -0.0736161066... |
707.1806 | Friction as a probe of surface properties of a polymer glass | We probe the temperature dependence of friction at the interface between a
glassy poly(methylmethacrylate) lens and a flat substrate coated with a
methyl-terminated self-assembled monolayer. The monolayer exhibits density
defects which act as pinning sites for the polymer chains. We show that the
shear response of su... | cond-mat.soft | we probe the temperature dependence of friction at the interface between a glassy polymethylmethacrylate lens and a flat substrate coated with a methylterminated selfassembled monolayer the monolayer exhibits density defects which act as pinning sites for the polymer chains we show that the shear response of such an in... | [['we', 'probe', 'the', 'temperature', 'dependence', 'of', 'friction', 'at', 'the', 'interface', 'between', 'a', 'glassy', 'polymethylmethacrylate', 'lens', 'and', 'a', 'flat', 'substrate', 'coated', 'with', 'a', 'methylterminated', 'selfassembled', 'monolayer', 'the', 'monolayer', 'exhibits', 'density', 'defects', 'wh... | [-0.18213395116109293, 0.22429326290699306, -0.09224636924398828, -0.05596900184286162, 0.009864257739006895, -0.17429237385976662, 0.048262706510180116, 0.4206703875430869, -0.30526475457348, -0.25710633994211235, 0.00925221299476813, -0.2918215225296981, -0.15444878739693646, 0.12947465209471223, 0.060246865097795005... |
707.1807 | Measurement of Scattering Rate and Minimum Conductivity in Graphene | The conductivity of graphene samples with various levels of disorder is
investigated for a set of specimens with mobility in the range of
$1-20\times10^3$ cm$^2$/V sec. Comparing the experimental data with the
theoretical transport calculations based on charged impurity scattering, we
estimate that the impurity conce... | cond-mat.mes-hall | the conductivity of graphene samples with various levels of disorder is investigated for a set of specimens with mobility in the range of 120times103 cm2v sec comparing the experimental data with the theoretical transport calculations based on charged impurity scattering we estimate that the impurity concentration in t... | [['the', 'conductivity', 'of', 'graphene', 'samples', 'with', 'various', 'levels', 'of', 'disorder', 'is', 'investigated', 'for', 'a', 'set', 'of', 'specimens', 'with', 'mobility', 'in', 'the', 'range', 'of', '120times103', 'cm2v', 'sec', 'comparing', 'the', 'experimental', 'data', 'with', 'the', 'theoretical', 'transp... | [-0.11212256597995826, 0.19831245778760778, -0.023266608177453553, 0.0009851401827699684, 0.05710634251270409, -0.07900255779231634, 0.058703069252585734, 0.39221433809864414, -0.22277176786863476, -0.3523199448720851, 0.04995460656937212, -0.37319918555301534, -0.042354774206915205, 0.17689667892249283, -0.02199377706... |
707.1808 | Universal L^s -rate-optimality of L^r-optimal quantizers by dilatation
and contraction | Let $ r, s>0 $. For a given probability measure $P$ on $\mathbb{R}^d$, let
$(\alpha_n)_{n \geq 1}$ be a sequence of (asymptotically) $L^r(P)$- optimal
quantizers. For all $\mu \in \mathbb{R}^d $ and for every $\theta >0$, one
defines the sequence $(\alpha_n^{\theta, \mu})_{n \geq 1}$ by : $\forall n \geq
1, \alpha_n^... | math.PR | let r s0 for a given probability measure p on mathbbrd let alpha_n_n geq 1 be a sequence of asymptotically lrp optimal quantizers for all mu in mathbbrd and for every theta 0 one defines the sequence alpha_ntheta mu_n geq 1 by forall n geq 1 alpha_ntheta mu mu thetaalpha_n mu mu thetaa mu a in alpha_n in this paper we ... | [['let', 'r', 's0', 'for', 'a', 'given', 'probability', 'measure', 'p', 'on', 'mathbbrd', 'let', 'alpha_n_n', 'geq', '1', 'be', 'a', 'sequence', 'of', 'asymptotically', 'lrp', 'optimal', 'quantizers', 'for', 'all', 'mu', 'in', 'mathbbrd', 'and', 'for', 'every', 'theta', '0', 'one', 'defines', 'the', 'sequence', 'alpha_... | [-0.15866026999886895, 0.17016825455500453, -0.04956196167613151, 0.06123051780359972, 0.05706587727715979, -0.19384151188748294, 0.048409179691797824, 0.3532652872381732, -0.2767095645340007, -0.20589092899052824, 0.049944960832840106, -0.33091697118199265, -0.07887255470840962, 0.13151777440827095, -0.069516425131682... |
707.1809 | The Overconvergent Site II. Cohomology | We prove that rigid cohomology can be computed as the cohomology of a site
analogous to the crystalline site. Berthelot designed rigid cohomology as a
common generalization of crystalline and Monsky-Washnitzer cohomology.
Unfortunately, unlike the former, the functoriality of the theory is not
built-in. We defined so... | math.AG | we prove that rigid cohomology can be computed as the cohomology of a site analogous to the crystalline site berthelot designed rigid cohomology as a common generalization of crystalline and monskywashnitzer cohomology unfortunately unlike the former the functoriality of the theory is not builtin we defined somewhere e... | [['we', 'prove', 'that', 'rigid', 'cohomology', 'can', 'be', 'computed', 'as', 'the', 'cohomology', 'of', 'a', 'site', 'analogous', 'to', 'the', 'crystalline', 'site', 'berthelot', 'designed', 'rigid', 'cohomology', 'as', 'a', 'common', 'generalization', 'of', 'crystalline', 'and', 'monskywashnitzer', 'cohomology', 'un... | [-0.17509439684480668, 0.03367104516154961, -0.13303732367292528, 0.08465165026255593, -0.09550005429854957, -0.1330619473711297, -0.013189733589521198, 0.36281481347176975, -0.40333207149899775, -0.18533335933061215, 0.1009319149438412, -0.17741481109612411, -0.13950206877122964, 0.19379586985795408, -0.20986712511168... |
707.181 | Measurement of the eta-Meson Mass using psi(2S) --> eta J/psi | We measure the mass of the eta meson using psi(2S) --> eta J/psi events
acquired with the CLEO-c detector operating at the CESR e+e- collider. Using
the four decay modes eta --> gamma gamma, 3pi0, pi+pi-pi0, and pi+pi-gamma, we
find M(eta)=547.785 +- 0.017 +- 0.057 MeV, in which the first uncertainty is
statistical a... | hep-ex | we measure the mass of the eta meson using psi2s eta jpsi events acquired with the cleoc detector operating at the cesr ee collider using the four decay modes eta gamma gamma 3pi0 pipipi0 and pipigamma we find meta547785 0017 0057 mev in which the first uncertainty is statistical and the second systematic this result h... | [['we', 'measure', 'the', 'mass', 'of', 'the', 'eta', 'meson', 'using', 'psi2s', 'eta', 'jpsi', 'events', 'acquired', 'with', 'the', 'cleoc', 'detector', 'operating', 'at', 'the', 'cesr', 'ee', 'collider', 'using', 'the', 'four', 'decay', 'modes', 'eta', 'gamma', 'gamma', '3pi0', 'pipipi0', 'and', 'pipigamma', 'we', 'f... | [-0.05417371798169122, 0.18538208385358634, -0.1207738007651642, 0.07290648558145305, -0.00912279016186155, -0.11438963071189144, 0.05832108118656007, 0.29869358491851017, -0.17280060185294133, -0.2850635316519236, -0.0078045087377011605, -0.4103867309167981, 0.0695022694919978, 0.22065459247096442, 0.04353653735862198... |
707.1811 | Caract\'erisation \'electromagn\'etique de milieux h\'et\'erog\`enes
naturels - Application \`a la mesure de l'humidit\'e du sol par radiom\'etrie
micro-onde | The work which we present takes place within the framework of mission SMOS of
the ESA which will consist to send a radiometer (1.4 GHz) in space. The goal of
the research which we propose is the improvement of the comprehension of the
effects of structure soil and litter. The effects of the litter and
heterogeneities... | physics.geo-ph | the work which we present takes place within the framework of mission smos of the esa which will consist to send a radiometer 14 ghz in space the goal of the research which we propose is the improvement of the comprehension of the effects of structure soil and litter the effects of the litter and heterogeneities of the... | [['the', 'work', 'which', 'we', 'present', 'takes', 'place', 'within', 'the', 'framework', 'of', 'mission', 'smos', 'of', 'the', 'esa', 'which', 'will', 'consist', 'to', 'send', 'a', 'radiometer', '14', 'ghz', 'in', 'space', 'the', 'goal', 'of', 'the', 'research', 'which', 'we', 'propose', 'is', 'the', 'improvement', '... | [-0.09922789556337996, 0.13801700022697438, -0.07962931060728475, 0.016989704025195517, -0.07393119221784338, -0.06868610635440606, 0.037451421175777475, 0.37140337502869375, -0.2308450207542492, -0.34331554653000657, 0.11785366974199993, -0.2515029550893708, -0.1372161079665483, 0.18470265936398755, -0.023968339749836... |
707.1812 | A numerical study of heat island flows in an open domain: Stationary
solutions | We present two dimensional numerical simulations of a natural convection
problem in an unbounded domain. A thermal stratification is applied in the
vertical direction and the flow circulation is induced by a heat island located
on the ground. For this problem, thermal perturbations are convected in the
horizontal dir... | math.NA cs.NA physics.class-ph | we present two dimensional numerical simulations of a natural convection problem in an unbounded domain a thermal stratification is applied in the vertical direction and the flow circulation is induced by a heat island located on the ground for this problem thermal perturbations are convected in the horizontal directio... | [['we', 'present', 'two', 'dimensional', 'numerical', 'simulations', 'of', 'a', 'natural', 'convection', 'problem', 'in', 'an', 'unbounded', 'domain', 'a', 'thermal', 'stratification', 'is', 'applied', 'in', 'the', 'vertical', 'direction', 'and', 'the', 'flow', 'circulation', 'is', 'induced', 'by', 'a', 'heat', 'island... | [-0.1288275403750694, 0.13326483209227893, -0.06141461310589798, 0.030707923455649398, -0.061227764982061506, -0.07316854611262043, 0.0072030871290649865, 0.39202400573935264, -0.3082528470251232, -0.2534229165563981, 0.1471193119740257, -0.27241081935472977, -0.060724707431772836, 0.19258835041969138, -0.0417031078702... |
707.1813 | Caracterisation Electromagnetique De Materiaux Geologiques En Vue Du
Suivi De L'Humidite Des Sols Par Radiometrie Micro-Ondes | The work which we present takes place within the framework of mission SMOS of
the ESA which will consist to send a radiometer (1.4 GHz) in space. The goal of
the research which we propose is the improvement of the comprehension of the
effects of structures composed of soil and litter. The effects of the litter
and he... | physics.geo-ph | the work which we present takes place within the framework of mission smos of the esa which will consist to send a radiometer 14 ghz in space the goal of the research which we propose is the improvement of the comprehension of the effects of structures composed of soil and litter the effects of the litter and heterogen... | [['the', 'work', 'which', 'we', 'present', 'takes', 'place', 'within', 'the', 'framework', 'of', 'mission', 'smos', 'of', 'the', 'esa', 'which', 'will', 'consist', 'to', 'send', 'a', 'radiometer', '14', 'ghz', 'in', 'space', 'the', 'goal', 'of', 'the', 'research', 'which', 'we', 'propose', 'is', 'the', 'improvement', '... | [-0.07898154931928159, 0.08766919365725283, -0.08883098379580998, -0.00394040829535525, -0.0605836476448899, -0.0461598362140601, 0.0496232949054246, 0.34382931262352107, -0.24407764336130783, -0.34198648896482253, 0.1175397694501965, -0.2676465370314914, -0.1336282506323377, 0.1573982757023152, -0.046285611992774936, ... |
707.1814 | Interference of multi-mode photon echoes generated in spatially
separated solid-state atomic ensembles | High-visibility interference of photon echoes generated in spatially
separated solid-state atomic ensembles is demonstrated. The solid state
ensembles were LiNbO$_3$ waveguides doped with Erbium ions absorbing at 1.53
$\mu$m. Bright coherent states of light in several temporal modes (up to 3) are
stored and retrieved... | quant-ph | highvisibility interference of photon echoes generated in spatially separated solidstate atomic ensembles is demonstrated the solid state ensembles were linbo_3 waveguides doped with erbium ions absorbing at 153 mum bright coherent states of light in several temporal modes up to 3 are stored and retrieved from the opti... | [['highvisibility', 'interference', 'of', 'photon', 'echoes', 'generated', 'in', 'spatially', 'separated', 'solidstate', 'atomic', 'ensembles', 'is', 'demonstrated', 'the', 'solid', 'state', 'ensembles', 'were', 'linbo_3', 'waveguides', 'doped', 'with', 'erbium', 'ions', 'absorbing', 'at', '153', 'mum', 'bright', 'cohe... | [-0.12797507691805152, 0.29960502789948473, -0.03843918523543383, 0.009590587211187836, 0.07486452002170657, -0.24129627868610104, 0.07002188337289474, 0.5165384301900371, -0.25033667344938626, -0.28649211791921253, 0.014978259834576367, -0.3392575849001565, -0.0337924811631164, 0.2305527174006378, -0.0162679720593016,... |
707.1815 | Etude D'Un Modele D'Inversion Liant L'Emissivite a L'Humidite Des Sols.
Contribution a la Mise Au Point De L'Algorithme De la Mission Smos | The work which we present takes place within the framework of mission SMOS of
the ESA which will consist to send a radiometer (1.4 GHz) in space. The goal of
the research which we propose is the improvement of the comprehension of the
effects of structure soil and litter. The effects of the litter and
heterogeneities... | physics.geo-ph | the work which we present takes place within the framework of mission smos of the esa which will consist to send a radiometer 14 ghz in space the goal of the research which we propose is the improvement of the comprehension of the effects of structure soil and litter the effects of the litter and heterogeneities of the... | [['the', 'work', 'which', 'we', 'present', 'takes', 'place', 'within', 'the', 'framework', 'of', 'mission', 'smos', 'of', 'the', 'esa', 'which', 'will', 'consist', 'to', 'send', 'a', 'radiometer', '14', 'ghz', 'in', 'space', 'the', 'goal', 'of', 'the', 'research', 'which', 'we', 'propose', 'is', 'the', 'improvement', '... | [-0.0763773854928428, 0.08999794842546838, -0.07889062429882308, 0.03181849956881513, -0.06737133468739054, -0.05031719702751713, 0.051380020939061376, 0.34682574590786974, -0.2442154784543202, -0.35102256745139654, 0.10825134954970092, -0.2556049559461052, -0.13849146783716007, 0.14203284926306298, -0.0385050177388388... |
707.1816 | Open FRW model in Loop Quantum Cosmology | Open FRW model in Loop Quantum Cosmology is under consideration. The left and
right invariant vector fields and holonomies along them are studied. It is
shown that in the hyperbolic geometry of $k=-1$ it is possible to construct a
suitable loop which provides us with quantum scalar constraint originally
introduced by... | gr-qc | open frw model in loop quantum cosmology is under consideration the left and right invariant vector fields and holonomies along them are studied it is shown that in the hyperbolic geometry of k1 it is possible to construct a suitable loop which provides us with quantum scalar constraint originally introduced by vanders... | [['open', 'frw', 'model', 'in', 'loop', 'quantum', 'cosmology', 'is', 'under', 'consideration', 'the', 'left', 'and', 'right', 'invariant', 'vector', 'fields', 'and', 'holonomies', 'along', 'them', 'are', 'studied', 'it', 'is', 'shown', 'that', 'in', 'the', 'hyperbolic', 'geometry', 'of', 'k1', 'it', 'is', 'possible', ... | [-0.1712508249840925, 0.20078673038744566, -0.08492183741746527, 0.09160116882853661, -0.14986903141393806, -0.27695701609252754, -0.07616312048666066, 0.352794313295321, -0.2630217377886628, -0.24793580902571027, 0.08580626446090525, -0.23532740967515786, -0.12752731415358456, 0.17117070713235685, -0.05405813801299893... |
707.1817 | HEIDI and the unparticle | We compare the HEIDI models with the unparticle models. We show that the
unparticle models are a limiting case of the HEIDI models. We discuss
consistency conditions.
| hep-ph | we compare the heidi models with the unparticle models we show that the unparticle models are a limiting case of the heidi models we discuss consistency conditions | [['we', 'compare', 'the', 'heidi', 'models', 'with', 'the', 'unparticle', 'models', 'we', 'show', 'that', 'the', 'unparticle', 'models', 'are', 'a', 'limiting', 'case', 'of', 'the', 'heidi', 'models', 'we', 'discuss', 'consistency', 'conditions']] | [-0.07238968723901996, 0.09169803777088721, -0.09205986980210852, 0.2241835220268479, -0.03299157748309275, -0.15007265689955265, -0.02363300585636386, 0.4201217845634178, -0.1738022661043538, -0.2378120382350904, 0.08674021860308669, -0.2779747618500281, -0.2115990905850022, 0.17090189456939697, 0.004927829218407472, ... |
707.1818 | Large continuum, oracles | Our main theorem is about iterated forcing for making the continuum larger
than aleph_2. We present a generalization of math.LO/0303294 which is dealing
with oracles for random, etc., replacing aleph_1, aleph_2 by lambda,lambda^+
(starting with lambda=lambda^{<lambda}>aleph_1). Well, instead of properness we
demand a... | math.LO | our main theorem is about iterated forcing for making the continuum larger than aleph_2 we present a generalization of mathlo0303294 which is dealing with oracles for random etc replacing aleph_1 aleph_2 by lambdalambda starting with lambdalambdalambdaaleph_1 well instead of properness we demand absolute ccc so we get ... | [['our', 'main', 'theorem', 'is', 'about', 'iterated', 'forcing', 'for', 'making', 'the', 'continuum', 'larger', 'than', 'aleph_2', 'we', 'present', 'a', 'generalization', 'of', 'mathlo0303294', 'which', 'is', 'dealing', 'with', 'oracles', 'for', 'random', 'etc', 'replacing', 'aleph_1', 'aleph_2', 'by', 'lambdalambda',... | [-0.09872087179748736, 0.11288260082176453, -0.09005232793475751, 0.11577310661201588, -0.13175988627571456, -0.17349666599381033, 0.05930369597544868, 0.4007083406855523, -0.2526205456881246, -0.2207664510523769, 0.14331034464518946, -0.29444782157808963, -0.09339912012744118, 0.16822220387124182, -0.1336029307051024,... |
707.1819 | One-way quantum computation via manipulation of polarization and
momentum qubits in two-photon cluster states | Four-qubit cluster states of two photons entangled in polarization and linear
momentum have been used to realize a complete set of single qubit rotations and
the C-NOT gate for equatorial qubits with high values of fidelity. By the
computational equivalence of the two degrees of freedom our result demonstrate
the sui... | quant-ph | fourqubit cluster states of two photons entangled in polarization and linear momentum have been used to realize a complete set of single qubit rotations and the cnot gate for equatorial qubits with high values of fidelity by the computational equivalence of the two degrees of freedom our result demonstrate the suitabil... | [['fourqubit', 'cluster', 'states', 'of', 'two', 'photons', 'entangled', 'in', 'polarization', 'and', 'linear', 'momentum', 'have', 'been', 'used', 'to', 'realize', 'a', 'complete', 'set', 'of', 'single', 'qubit', 'rotations', 'and', 'the', 'cnot', 'gate', 'for', 'equatorial', 'qubits', 'with', 'high', 'values', 'of', ... | [-0.16717755770872508, 0.21776603939869102, -0.010703589264599104, -0.01245012059290376, 0.04907157758457793, -0.191864557505127, 0.09548142519114274, 0.397761988024863, -0.19633910802030374, -0.336833942533722, 0.018898149263039822, -0.23191454475154244, -0.011671746164442056, 0.24196651261595506, -0.01184103739935727... |
707.182 | Understanding the Properties of the BitTorrent Overlay | In this paper, we conduct extensive simulations to understand the properties
of the overlay generated by BitTorrent. We start by analyzing how the overlay
properties impact the efficiency of BitTorrent. We focus on the average peer
set size (i.e., average number of neighbors), the time for a peer to reach its
maximum... | cs.NI | in this paper we conduct extensive simulations to understand the properties of the overlay generated by bittorrent we start by analyzing how the overlay properties impact the efficiency of bittorrent we focus on the average peer set size ie average number of neighbors the time for a peer to reach its maximum peer set s... | [['in', 'this', 'paper', 'we', 'conduct', 'extensive', 'simulations', 'to', 'understand', 'the', 'properties', 'of', 'the', 'overlay', 'generated', 'by', 'bittorrent', 'we', 'start', 'by', 'analyzing', 'how', 'the', 'overlay', 'properties', 'impact', 'the', 'efficiency', 'of', 'bittorrent', 'we', 'focus', 'on', 'the', ... | [-0.18792183964056802, 0.08515694331709701, -0.04859724722913291, 0.007873688821593245, -0.10198722215078881, -0.0784774294081559, 0.17063191972758235, 0.3992695928537425, -0.2686755058498555, -0.3047601947339602, 0.060846664852319786, -0.3198772463394274, -0.15804634255986422, 0.1171171494049601, -0.06014611208776823,... |
707.1821 | Emergence of scale-free behavior in networks from limited-horizon
linking and cost trade-offs | We study network growth from a fixed set of initially isolated nodes placed
at random on the surface of a sphere. The growth mechanism we use adds edges to
the network depending on strictly local gain and cost criteria. Only nodes that
are not too far apart on the sphere may be considered for being joined by an
edge.... | cond-mat.stat-mech | we study network growth from a fixed set of initially isolated nodes placed at random on the surface of a sphere the growth mechanism we use adds edges to the network depending on strictly local gain and cost criteria only nodes that are not too far apart on the sphere may be considered for being joined by an edge give... | [['we', 'study', 'network', 'growth', 'from', 'a', 'fixed', 'set', 'of', 'initially', 'isolated', 'nodes', 'placed', 'at', 'random', 'on', 'the', 'surface', 'of', 'a', 'sphere', 'the', 'growth', 'mechanism', 'we', 'use', 'adds', 'edges', 'to', 'the', 'network', 'depending', 'on', 'strictly', 'local', 'gain', 'and', 'co... | [-0.16310178929677185, 0.12009298623898082, -0.057535373898318566, 0.00730477388536271, -0.08711525246214408, -0.16803584038876954, 0.11171317241865043, 0.38925328104792595, -0.25985385473363865, -0.273798118894681, 0.07782545065707289, -0.31333888325696957, -0.13521547336579084, 0.17588181927865848, -0.025495267323910... |
707.1822 | FIRI - a Far-Infrared Interferometer | Half of the energy ever emitted by stars and accreting objects comes to us in
the FIR waveband and has yet to be properly explored. We propose a powerful
Far-InfraRed Interferometer mission, FIRI, to carry out high-resolution imaging
spectroscopy in the FIR. This key observational capability is essential to
reveal ho... | astro-ph | half of the energy ever emitted by stars and accreting objects comes to us in the fir waveband and has yet to be properly explored we propose a powerful farinfrared interferometer mission firi to carry out highresolution imaging spectroscopy in the fir this key observational capability is essential to reveal how gas an... | [['half', 'of', 'the', 'energy', 'ever', 'emitted', 'by', 'stars', 'and', 'accreting', 'objects', 'comes', 'to', 'us', 'in', 'the', 'fir', 'waveband', 'and', 'has', 'yet', 'to', 'be', 'properly', 'explored', 'we', 'propose', 'a', 'powerful', 'farinfrared', 'interferometer', 'mission', 'firi', 'to', 'carry', 'out', 'hig... | [-0.040580830123220904, 0.12833418130564192, -0.10506415916434317, 0.13721396972588407, -0.14365760489068005, -0.04818068529525197, 0.015502273853879743, 0.3903507948335674, -0.17721879384322323, -0.3477357770373792, 0.07833605998534893, -0.2807515944428972, -0.09476275381597656, 0.19225286401609834, -0.070111936033002... |
707.1823 | Lband radiometric behaviour of pine forests for a variety of surface
moisture conditions | From July-December 2004 the experimental campaign 'Bray 2004' was conducted
in the coniferous forest of Les Landes near Bordeaux, France, using a
multi-angle L-band (1.4 GHz) radiometer to measure upwelling radiation above
the forest. At the same time, ground measurements were taken of soil and litter
moisture conten... | physics.geo-ph | from julydecember 2004 the experimental campaign bray 2004 was conducted in the coniferous forest of les landes near bordeaux france using a multiangle lband 14 ghz radiometer to measure upwelling radiation above the forest at the same time ground measurements were taken of soil and litter moisture content this experim... | [['from', 'julydecember', '2004', 'the', 'experimental', 'campaign', 'bray', '2004', 'was', 'conducted', 'in', 'the', 'coniferous', 'forest', 'of', 'les', 'landes', 'near', 'bordeaux', 'france', 'using', 'a', 'multiangle', 'lband', '14', 'ghz', 'radiometer', 'to', 'measure', 'upwelling', 'radiation', 'above', 'the', 'f... | [-0.05982623632591103, 0.1157841699737399, -0.07935679557408448, 0.01972450530141108, -0.05523786402721828, -0.07377722906769307, 0.048186772375517335, 0.3491148178584644, -0.20451927061155767, -0.3362321585318328, 0.16934881578886773, -0.31730184602932715, -0.10962432353923483, 0.1884570064603675, -0.0335908942642552,... |
707.1824 | The Kinematics of Manipulators Built From Closed Planar Mechanisms | The paper discusses the kinematics of manipulators builts of planar closed
kinematic chains. A special kinematic scheme is extracted from the array of
these mechanisms that looks the most promising for the creation of different
types of robotic manipulators. The structural features of this manipulator
determine a num... | cs.RO | the paper discusses the kinematics of manipulators builts of planar closed kinematic chains a special kinematic scheme is extracted from the array of these mechanisms that looks the most promising for the creation of different types of robotic manipulators the structural features of this manipulator determine a number ... | [['the', 'paper', 'discusses', 'the', 'kinematics', 'of', 'manipulators', 'builts', 'of', 'planar', 'closed', 'kinematic', 'chains', 'a', 'special', 'kinematic', 'scheme', 'is', 'extracted', 'from', 'the', 'array', 'of', 'these', 'mechanisms', 'that', 'looks', 'the', 'most', 'promising', 'for', 'the', 'creation', 'of',... | [-0.1510540161834797, 0.027827813148698106, -0.0984492307574588, -0.0002453603576993503, -0.12020634915513385, -0.14463213952175075, -0.007731909184907896, 0.37287341873161495, -0.2878246547573196, -0.3188591633599052, 0.09234625679839935, -0.18305676208651026, -0.17391856618009374, 0.22188518968011653, -0.047806511724... |
707.1825 | A solid angle polynomial with negative coefficients | This article has been replaced by arXiv:0906.4031
| math.CO | this article has been replaced by arxiv09064031 | [['this', 'article', 'has', 'been', 'replaced', 'by', 'arxiv09064031']] | [-0.04845165212949117, 0.13359238533303142, -0.13563921042562774, -0.12186264442667986, -0.05646844394505024, -0.11079728199789922, -0.0883878383707876, 0.3959589848915736, -0.16523358598351479, -0.2645369420448939, 0.20824163407087326, -0.2495188762744268, -0.18675473487625519, 0.1293863651032249, -0.2036297246813774,... |
707.1826 | Doping-driven Mott transition in La_{1-x}Sr_xTiO_3 via simultaneous
electron and hole doping of t2g subbands | The insulator to metal transition in LaTiO_3 induced by La substitution via
Sr is studied within multi-band exact diagonalization dynamical mean field
theory at finite temperatures. It is shown that weak hole doping triggers a
large interorbital charge transfer, with simultaneous electron and hole doping
of t2g subba... | cond-mat.str-el | the insulator to metal transition in latio_3 induced by la substitution via sr is studied within multiband exact diagonalization dynamical mean field theory at finite temperatures it is shown that weak hole doping triggers a large interorbital charge transfer with simultaneous electron and hole doping of t2g subbands t... | [['the', 'insulator', 'to', 'metal', 'transition', 'in', 'latio_3', 'induced', 'by', 'la', 'substitution', 'via', 'sr', 'is', 'studied', 'within', 'multiband', 'exact', 'diagonalization', 'dynamical', 'mean', 'field', 'theory', 'at', 'finite', 'temperatures', 'it', 'is', 'shown', 'that', 'weak', 'hole', 'doping', 'trig... | [-0.1805016736253303, 0.23132189232893496, -0.0035069556215243172, 0.08881682398991825, 0.0031014018263298983, -0.21370026841413894, 0.10152855786923688, 0.4031099715260881, -0.25349936034014026, -0.266501889029278, -0.04397743100318873, -0.3518451539762687, -0.10108434605310754, 0.12539137507924847, 0.0258182504163630... |
707.1827 | Magnetospheric Emissions from the Planet Orbiting tau Boo: A Multi-Epoch
Search | All of the solar system gas giants produce electron cyclotron masers, driven
by the solar wind impinging on their magnetospheres. Extrapolating to the
planet orbiting tau Boo, various authors have predicted that it may be within
the detection limits of the 4-meter wavelength (74 MHz) system on the Very
Large Array. T... | astro-ph | all of the solar system gas giants produce electron cyclotron masers driven by the solar wind impinging on their magnetospheres extrapolating to the planet orbiting tau boo various authors have predicted that it may be within the detection limits of the 4meter wavelength 74 mhz system on the very large array this paper... | [['all', 'of', 'the', 'solar', 'system', 'gas', 'giants', 'produce', 'electron', 'cyclotron', 'masers', 'driven', 'by', 'the', 'solar', 'wind', 'impinging', 'on', 'their', 'magnetospheres', 'extrapolating', 'to', 'the', 'planet', 'orbiting', 'tau', 'boo', 'various', 'authors', 'have', 'predicted', 'that', 'it', 'may', ... | [-0.08220970754903277, 0.17113563566075085, -0.029810274771909583, 0.06727442877156714, -0.10070412350471704, -0.10895173295856957, 0.047474519363760355, 0.3960991613001847, -0.17761384222118737, -0.37917260263917896, 0.09810943224588624, -0.2815270776846777, 0.0020436311849864456, 0.24450020108247278, -0.0239203680330... |
707.1828 | An extended version of additive K-theory | There are two infinitesimal (i.e., additive) versions of the $K$-theory of a
field $F$: one was introduced by Cathelineau, which is an $F$-module, and
another one introduced by Bloch-Esnault, which is an $F^*$-module. Both
versions are equipped with a regulator map, when $F$ is the field of complex
numbers.
In our ... | math.AG math.NT | there are two infinitesimal ie additive versions of the ktheory of a field f one was introduced by cathelineau which is an fmodule and another one introduced by blochesnault which is an fmodule both versions are equipped with a regulator map when f is the field of complex numbers in our short paper we will introduce an... | [['there', 'are', 'two', 'infinitesimal', 'ie', 'additive', 'versions', 'of', 'the', 'ktheory', 'of', 'a', 'field', 'f', 'one', 'was', 'introduced', 'by', 'cathelineau', 'which', 'is', 'an', 'fmodule', 'and', 'another', 'one', 'introduced', 'by', 'blochesnault', 'which', 'is', 'an', 'fmodule', 'both', 'versions', 'are'... | [-0.16530535878521985, 0.09096523021196576, -0.10604265153972951, 0.06330877542734284, -0.06920427200002749, -0.119168387260288, -0.02106046673486803, 0.3344432248077432, -0.28341245913465857, -0.24365780284231314, 0.1318577582915466, -0.25730323057944243, -0.1864065167586678, 0.2205841884810905, -0.1306029390534157, -... |
707.1829 | Dirac equation: Representation independence and tensor transformation | We define and study the probability current and the Hamiltonian operator for
a fully general set of Dirac matrices in a flat spacetime with affine
coordinates, by using the Bargmann-Pauli hermitizing matrix. We find that with
some weak conditions on the affine coordinates, the current, as well as the
spectrum of the ... | quant-ph gr-qc hep-th | we define and study the probability current and the hamiltonian operator for a fully general set of dirac matrices in a flat spacetime with affine coordinates by using the bargmannpauli hermitizing matrix we find that with some weak conditions on the affine coordinates the current as well as the spectrum of the dirac h... | [['we', 'define', 'and', 'study', 'the', 'probability', 'current', 'and', 'the', 'hamiltonian', 'operator', 'for', 'a', 'fully', 'general', 'set', 'of', 'dirac', 'matrices', 'in', 'a', 'flat', 'spacetime', 'with', 'affine', 'coordinates', 'by', 'using', 'the', 'bargmannpauli', 'hermitizing', 'matrix', 'we', 'find', 'th... | [-0.13128850297371467, 0.12333096158615645, -0.059887296580258875, 0.027918849670846436, -0.105412598137909, -0.13306502881459892, -0.010991852448862647, 0.3129756044025623, -0.27210682034943134, -0.2204983250093421, 0.06575639566102426, -0.26539530058301264, -0.20392736133878991, 0.15124511302659108, -0.00477721301778... |
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