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 |
|---|---|---|---|---|---|---|
708.2849 | Orientation Dependence of the Anomalous Hall Resistivity in Single
Crystals of Yb14MnSb11 | The Hall resistivity, electrical resistivity and magnetization of single
crystals of the tetragonal ferromagnet Yb14MnSb11 are reported as a function of
the direction of the current, I, and magnetic field, H with respect to the
principal crystallographic axes. With I along the unique c direction and H in
the a-b plan... | cond-mat.str-el | the hall resistivity electrical resistivity and magnetization of single crystals of the tetragonal ferromagnet yb14mnsb11 are reported as a function of the direction of the current i and magnetic field h with respect to the principal crystallographic axes with i along the unique c direction and h in the ab plane the an... | [['the', 'hall', 'resistivity', 'electrical', 'resistivity', 'and', 'magnetization', 'of', 'single', 'crystals', 'of', 'the', 'tetragonal', 'ferromagnet', 'yb14mnsb11', 'are', 'reported', 'as', 'a', 'function', 'of', 'the', 'direction', 'of', 'the', 'current', 'i', 'and', 'magnetic', 'field', 'h', 'with', 'respect', 't... | [-0.16918284945314296, 0.19625483387727566, -0.027415618380551697, -0.03001152294208913, -0.09846653329545639, -0.14790392338755579, 0.051356244667042646, 0.391098624900631, -0.2901732566896626, -0.26239362178728365, 0.04036939854142807, -0.31875484217772776, -0.08229514549730019, 0.22656792497736364, 0.029835994709633... |
708.285 | Efficient strong integrators for linear stochastic systems | We present numerical schemes for the strong solution of linear stochastic
differential equations driven by an arbitrary number of Wiener processes. These
schemes are based on the Neumann (stochastic Taylor) and Magnus expansions.
Firstly, we consider the case when the governing linear diffusion vector fields
commute ... | math.NA | we present numerical schemes for the strong solution of linear stochastic differential equations driven by an arbitrary number of wiener processes these schemes are based on the neumann stochastic taylor and magnus expansions firstly we consider the case when the governing linear diffusion vector fields commute with ea... | [['we', 'present', 'numerical', 'schemes', 'for', 'the', 'strong', 'solution', 'of', 'linear', 'stochastic', 'differential', 'equations', 'driven', 'by', 'an', 'arbitrary', 'number', 'of', 'wiener', 'processes', 'these', 'schemes', 'are', 'based', 'on', 'the', 'neumann', 'stochastic', 'taylor', 'and', 'magnus', 'expans... | [-0.13921635874886015, 0.06579654056743796, -0.04256743907953809, 0.07446994990835815, -0.09775586558037064, -0.12120220243461988, -0.0038851610793523036, 0.3511891402921887, -0.32234505206809005, -0.20862246070335916, 0.13676240670314171, -0.23260464694439656, -0.17776000915019183, 0.25149994995603403, -0.059164314087... |
708.2851 | Functoriality for Lagrangian correspondences in Floer theory | Using quilted Floer cohomology and relative quilt invariants, we define a
composition functor for categories of Lagrangian correspondences in monotone
and exact symplectic Floer theory. We show that this functor agrees with
geometric composition in the case that the composition is smooth and embedded.
As a consequenc... | math.SG math.DG | using quilted floer cohomology and relative quilt invariants we define a composition functor for categories of lagrangian correspondences in monotone and exact symplectic floer theory we show that this functor agrees with geometric composition in the case that the composition is smooth and embedded as a consequence we ... | [['using', 'quilted', 'floer', 'cohomology', 'and', 'relative', 'quilt', 'invariants', 'we', 'define', 'a', 'composition', 'functor', 'for', 'categories', 'of', 'lagrangian', 'correspondences', 'in', 'monotone', 'and', 'exact', 'symplectic', 'floer', 'theory', 'we', 'show', 'that', 'this', 'functor', 'agrees', 'with', ... | [-0.17639551680102677, 0.029237533204390535, -0.16020095163756715, 0.10860457238075989, -0.0624907983250783, -0.1070677036685603, -0.06501024170886792, 0.3795546438611512, -0.39674740048524526, -0.27593876158685554, -0.0002653389029936599, -0.1965323602967796, -0.22590479873386876, 0.1183800742146559, -0.26426535488904... |
708.2852 | Modeling Non-Circular Motions in Disk Galaxies: A Bar in NGC 2976 | We give a brief description of a new model for non-circular motions in disk
galaxy velocity fields, that does not invoke epicycles. We assume non-circular
motions to stem from a bar-like or oval distortion to the potential, as could
arise from a triaxial halo or a bar in the mass distribution of the baryons. We
apply... | astro-ph | we give a brief description of a new model for noncircular motions in disk galaxy velocity fields that does not invoke epicycles we assume noncircular motions to stem from a barlike or oval distortion to the potential as could arise from a triaxial halo or a bar in the mass distribution of the baryons we apply our mode... | [['we', 'give', 'a', 'brief', 'description', 'of', 'a', 'new', 'model', 'for', 'noncircular', 'motions', 'in', 'disk', 'galaxy', 'velocity', 'fields', 'that', 'does', 'not', 'invoke', 'epicycles', 'we', 'assume', 'noncircular', 'motions', 'to', 'stem', 'from', 'a', 'barlike', 'or', 'oval', 'distortion', 'to', 'the', 'p... | [-0.06993594509740284, 0.03999230027061383, -0.1552202251556589, 0.09493237909036459, -0.1394023346355887, -0.0716441786909079, 0.023010791204946084, 0.38683894911750416, -0.183951437293903, -0.33525831559596614, 0.008497981379404053, -0.24887992407302142, -0.07688760310296947, 0.1900202703297703, -0.058895897944686845... |
708.2853 | Dense sets of integers with prescribed representation functions | Let A be a set of integers and let h \geq 2. For every integer n, let r_{A,
h}(n) denote the number of representations of n in the form n=a_1+...+a_h,
where a_1,...,a_h belong to the set A, and a_1\leq ... \leq a_h. The function
r_{A,h} from the integers Z to the nonnegative integers N_0 U {\infty} is
called the repr... | math.NT math.CO | let a be a set of integers and let h geq 2 for every integer n let r_a hn denote the number of representations of n in the form na_1a_h where a_1a_h belong to the set a and a_1leq leq a_h the function r_ah from the integers z to the nonnegative integers n_0 u infty is called the representation function of order h for t... | [['let', 'a', 'be', 'a', 'set', 'of', 'integers', 'and', 'let', 'h', 'geq', '2', 'for', 'every', 'integer', 'n', 'let', 'r_a', 'hn', 'denote', 'the', 'number', 'of', 'representations', 'of', 'n', 'in', 'the', 'form', 'na_1a_h', 'where', 'a_1a_h', 'belong', 'to', 'the', 'set', 'a', 'and', 'a_1leq', 'leq', 'a_h', 'the', ... | [-0.18299670560039985, 0.163226703649329, -0.049820723149261274, -0.021265904475075675, -0.02405692515317206, -0.17368918105728867, 0.009000816312979531, 0.32390288003655365, -0.3207600245237813, -0.23820163355779278, 0.04360728015827174, -0.33735267696685567, -0.09134082908763788, 0.14717503828393627, -0.0049020973893... |
708.2854 | Algorithmic Semi-algebraic Geometry and Topology -- Recent Progress and
Open Problems | We give a survey of algorithms for computing topological invariants of
semi-algebraic sets with special emphasis on the more recent developments in
designing algorithms for computing the Betti numbers of semi-algebraic sets.
Aside from describing these results, we discuss briefly the background as well
as the importa... | math.GT cs.CC cs.CG math.AG math.AT | we give a survey of algorithms for computing topological invariants of semialgebraic sets with special emphasis on the more recent developments in designing algorithms for computing the betti numbers of semialgebraic sets aside from describing these results we discuss briefly the background as well as the importance of... | [['we', 'give', 'a', 'survey', 'of', 'algorithms', 'for', 'computing', 'topological', 'invariants', 'of', 'semialgebraic', 'sets', 'with', 'special', 'emphasis', 'on', 'the', 'more', 'recent', 'developments', 'in', 'designing', 'algorithms', 'for', 'computing', 'the', 'betti', 'numbers', 'of', 'semialgebraic', 'sets', ... | [-0.1134226534393234, 0.04043650350724466, -0.04816630224768932, 0.11836203728587581, -0.0918365757052715, -0.10167500192824847, 0.04487044661520766, 0.32676532881286663, -0.2943930961191654, -0.31672537784116006, 0.18233275027700868, -0.24331657931459352, -0.2056419764740918, 0.31156100858098423, -0.10167675529821561,... |
708.2855 | Ettore Majorana's Scientific (and Human) Personality | This article, in English, represents part of the invited talk delivered by
the author at the "Internat.Conf.Majorana Legacy and Phys. XXI century" held at
Dep. of Phys.,University of Catania, Italy, in Oct.2006: Conference organized
for celebrating the 100th anniversary of the birth (in Catania) of the Italian
theore... | physics.hist-ph physics.ed-ph | this article in english represents part of the invited talk delivered by the author at the internatconfmajorana legacy and phys xxi century held at dep of physuniversity of catania italy in oct2006 conference organized for celebrating the 100th anniversary of the birth in catania of the italian theoretical physicist et... | [['this', 'article', 'in', 'english', 'represents', 'part', 'of', 'the', 'invited', 'talk', 'delivered', 'by', 'the', 'author', 'at', 'the', 'internatconfmajorana', 'legacy', 'and', 'phys', 'xxi', 'century', 'held', 'at', 'dep', 'of', 'physuniversity', 'of', 'catania', 'italy', 'in', 'oct2006', 'conference', 'organized... | [-0.09274065534753556, 0.0787770690747186, -0.04551593057415146, 0.08306248725184796, -0.08244205909318521, -0.23875900019903656, 0.047610765437946304, 0.17793863574451127, -0.07731065832346061, -0.3465321138017363, 0.022897870740407243, -0.42424867843888553, -0.08484141483174201, 0.1405970238499924, -0.226593038980401... |
708.2856 | Theoretical analysis of magnetic coupling in sandwich clusters
V_n(C_6H_6)_{n+1} | The mechanism of ferromagnetism stability in sandwich clusters
V$_n$(C$_6$H$_6$)$_{n+1}$ has been studied by first-principles calculation and
model analysis. It is found that each of the three types of bonds between V and
benzene (Bz) plays different roles. V 3d$_{z^2}$ orbital, extending along the
molecular axis, is... | cond-mat.mtrl-sci | the mechanism of ferromagnetism stability in sandwich clusters v_nc_6h_6_n1 has been studied by firstprinciples calculation and model analysis it is found that each of the three types of bonds between v and benzene bz plays different roles v 3d_z2 orbital extending along the molecular axis is weakly hybridized with bzs... | [['the', 'mechanism', 'of', 'ferromagnetism', 'stability', 'in', 'sandwich', 'clusters', 'v_nc_6h_6_n1', 'has', 'been', 'studied', 'by', 'firstprinciples', 'calculation', 'and', 'model', 'analysis', 'it', 'is', 'found', 'that', 'each', 'of', 'the', 'three', 'types', 'of', 'bonds', 'between', 'v', 'and', 'benzene', 'bz'... | [-0.1845514847620643, 0.14714328992398398, -0.004560110595979767, 0.04582589593222017, -0.04808337946050304, -0.13425652759267173, 0.08595072758241522, 0.3750331517892115, -0.26160328241857206, -0.3030697913344288, -0.0426537282019636, -0.31112035613715927, -0.1137321265947474, 0.10239766880425964, 0.056607067357056784... |
708.2857 | Spatial image of reaction area from scattering I: SO_mu(2.1) algebra
formalism | We develop general formalism of how to relate scattering amplitudes for
exclusive processes to spatial image of target hadron. More precisely we show
how to determine the spatial distribution of outgoing particles in the space of
so-called nearest approach parameter. This parameter characterizes the position
in the c... | hep-ph | we develop general formalism of how to relate scattering amplitudes for exclusive processes to spatial image of target hadron more precisely we show how to determine the spatial distribution of outgoing particles in the space of socalled nearest approach parameter this parameter characterizes the position in the coordi... | [['we', 'develop', 'general', 'formalism', 'of', 'how', 'to', 'relate', 'scattering', 'amplitudes', 'for', 'exclusive', 'processes', 'to', 'spatial', 'image', 'of', 'target', 'hadron', 'more', 'precisely', 'we', 'show', 'how', 'to', 'determine', 'the', 'spatial', 'distribution', 'of', 'outgoing', 'particles', 'in', 'th... | [-0.06399699792943961, 0.17980540182702898, -0.1384403107916577, 0.12279267435109145, -0.06982756018017729, -0.07822053795353624, 0.022126126560594952, 0.35989034927466457, -0.27353948523012694, -0.2506707426356642, -0.01653256030802272, -0.22464837862603498, -0.09704708151127163, 0.10951409787307248, -0.00607111925880... |
708.2858 | Dimer diffusion in a washboard potential | The transport of a dimer, consisting of two Brownian particles bounded by a
harmonic potential, moving on a periodic substrate is investigated both
numerically and analytically. The mobility and diffusion of the dimer center of
mass present distinct properties when compared with those of a monomer under
the same tran... | cond-mat.stat-mech | the transport of a dimer consisting of two brownian particles bounded by a harmonic potential moving on a periodic substrate is investigated both numerically and analytically the mobility and diffusion of the dimer center of mass present distinct properties when compared with those of a monomer under the same transport... | [['the', 'transport', 'of', 'a', 'dimer', 'consisting', 'of', 'two', 'brownian', 'particles', 'bounded', 'by', 'a', 'harmonic', 'potential', 'moving', 'on', 'a', 'periodic', 'substrate', 'is', 'investigated', 'both', 'numerically', 'and', 'analytically', 'the', 'mobility', 'and', 'diffusion', 'of', 'the', 'dimer', 'cen... | [-0.16629365672981675, 0.18844656344339417, -0.028766873896449476, 0.014864913281309162, 0.007356119334472568, -0.13308583928661033, -0.006230937843121445, 0.40587125440220256, -0.2805242427000469, -0.24110508688653892, 0.05720804327686962, -0.2762530696831623, -0.13041797838081698, 0.17638428894045588, 0.0653854312968... |
708.2859 | Studies of self-organized Nanostructures on InP(111) surfaces after low
energy Ar+ ion irradiation | We report formation of self organized InP nano dots using 3 keV Ar+ ion
sputtering, at $15^\circ$ incidence from surface normal, on InP(111) surface.
Morphology and optical properties of the sputtered surface, as a function of
sputtering time, have been investigated by Scanning Probe Microscopy and Raman
Scattering t... | cond-mat.mtrl-sci | we report formation of self organized inp nano dots using 3 kev ar ion sputtering at 15circ incidence from surface normal on inp111 surface morphology and optical properties of the sputtered surface as a function of sputtering time have been investigated by scanning probe microscopy and raman scattering techniques unif... | [['we', 'report', 'formation', 'of', 'self', 'organized', 'inp', 'nano', 'dots', 'using', '3', 'kev', 'ar', 'ion', 'sputtering', 'at', '15circ', 'incidence', 'from', 'surface', 'normal', 'on', 'inp111', 'surface', 'morphology', 'and', 'optical', 'properties', 'of', 'the', 'sputtered', 'surface', 'as', 'a', 'function', ... | [-0.06797499533140046, 0.2680189021753476, -0.03258109288427102, -0.012559000128770577, 0.04027629679288058, -0.15906985687872613, 0.04979069214553901, 0.46690202287453064, -0.2909510684254415, -0.3738079888978973, 0.03135694822104757, -0.31830895683344673, -0.04399472676655825, 0.22865941880051704, 0.01662369399495861... |
708.286 | Three-loop Corrections in a Covariant Effective Field Theory | Chiral effective field theories have been used with success in the study of
nuclear structure. It is of interest to systematically improve these energy
functionals (particularly that of quantum hadrodynamics) through the inclusion
of many-body correlations. One possible source of improvement is the loop
expansion. Us... | nucl-th | chiral effective field theories have been used with success in the study of nuclear structure it is of interest to systematically improve these energy functionals particularly that of quantum hadrodynamics through the inclusion of manybody correlations one possible source of improvement is the loop expansion using the ... | [['chiral', 'effective', 'field', 'theories', 'have', 'been', 'used', 'with', 'success', 'in', 'the', 'study', 'of', 'nuclear', 'structure', 'it', 'is', 'of', 'interest', 'to', 'systematically', 'improve', 'these', 'energy', 'functionals', 'particularly', 'that', 'of', 'quantum', 'hadrodynamics', 'through', 'the', 'inc... | [-0.1278542625764776, 0.18545340406982339, -0.1264867686745789, 0.12198146593271747, -0.0343137527307292, -0.0867496545410895, -0.019493606370020688, 0.3405083919397923, -0.24028363677931308, -0.29077541941636, 0.05161172322275415, -0.28429601202570215, -0.11965250865039768, 0.12866545067229426, 0.043935185673983156, 0... |
708.2861 | Poisson sigma models on surfaces with boundary: classical and quantum
aspects | The topics covered in this thesis may be divided into three parts. Firstly,
we perform a study on the most general branes which are consistent with the
Poisson sigma model, both at the classical and quantum levels. The second part
is devoted to the particular case in which the target Poisson manifold is a
Poisson-Lie... | hep-th math.DG math.QA | the topics covered in this thesis may be divided into three parts firstly we perform a study on the most general branes which are consistent with the poisson sigma model both at the classical and quantum levels the second part is devoted to the particular case in which the target poisson manifold is a poissonlie group ... | [['the', 'topics', 'covered', 'in', 'this', 'thesis', 'may', 'be', 'divided', 'into', 'three', 'parts', 'firstly', 'we', 'perform', 'a', 'study', 'on', 'the', 'most', 'general', 'branes', 'which', 'are', 'consistent', 'with', 'the', 'poisson', 'sigma', 'model', 'both', 'at', 'the', 'classical', 'and', 'quantum', 'level... | [-0.09118873806131121, 0.0775874113713048, -0.06640103527369272, 0.08892804294316049, -0.0728719183488896, -0.12569285438420544, -0.022674543222436977, 0.33089646010806684, -0.2690901210436622, -0.2457775348969, 0.10740237848949619, -0.25507959452653794, -0.18739445973187685, 0.1437560292389734, -0.09057430958828742, -... |
708.2862 | Quasi two-dimensional carriers in dilute-magnetic-semiconductor quantum
wells under in-plane magnetic field | Due to the competition between spatial and magnetic confinement, the density
of states of a quasi two-dimensional system deviates from the ideal step-like
form both quantitatively and qualitatively. We study how this affects the
spin-subband populations and the spin-polarization as functions of the
temperature, $T$, ... | cond-mat.mtrl-sci | due to the competition between spatial and magnetic confinement the density of states of a quasi twodimensional system deviates from the ideal steplike form both quantitatively and qualitatively we study how this affects the spinsubband populations and the spinpolarization as functions of the temperature t and the inpl... | [['due', 'to', 'the', 'competition', 'between', 'spatial', 'and', 'magnetic', 'confinement', 'the', 'density', 'of', 'states', 'of', 'a', 'quasi', 'twodimensional', 'system', 'deviates', 'from', 'the', 'ideal', 'steplike', 'form', 'both', 'quantitatively', 'and', 'qualitatively', 'we', 'study', 'how', 'this', 'affects'... | [-0.16351097871250073, 0.22842570880727311, -0.013189668684000415, 0.04997885297052562, 0.005253943680194035, -0.14042088264250197, 0.06790858755370469, 0.35643247445113957, -0.2939789712129693, -0.3039747297755509, -0.01586590100695113, -0.30733237678318154, -0.09603935807743776, 0.15497504616256005, 0.059021246465688... |
708.2863 | The Arecibo Methanol Maser Galactic Plane Survey - II: Statistical and
Multi-wavelength Counterpart Analysis | We present an analysis of the properties of the 6.7 GHz methanol maser sample
detected in the Arecibo Methanol Maser Galactic Plane Survey. The distribution
of the masers in the Galaxy, and statistics of their multi-wavelength
counterparts is consistent with the hypothesis of 6.7 GHz maser emission being
associated w... | astro-ph | we present an analysis of the properties of the 67 ghz methanol maser sample detected in the arecibo methanol maser galactic plane survey the distribution of the masers in the galaxy and statistics of their multiwavelength counterparts is consistent with the hypothesis of 67 ghz maser emission being associated with mas... | [['we', 'present', 'an', 'analysis', 'of', 'the', 'properties', 'of', 'the', '67', 'ghz', 'methanol', 'maser', 'sample', 'detected', 'in', 'the', 'arecibo', 'methanol', 'maser', 'galactic', 'plane', 'survey', 'the', 'distribution', 'of', 'the', 'masers', 'in', 'the', 'galaxy', 'and', 'statistics', 'of', 'their', 'multi... | [-0.09184747387989774, 0.02764259339319324, -0.04681402935530059, 0.02869873289309908, -0.11319778804318048, -0.030915770612773487, 0.0451823871160741, 0.4378463213608484, -0.12270624298689654, -0.31458344265120103, 0.06326870070406584, -0.28186416064854714, -0.03358063981831947, 0.1859768394380808, 0.02214057211967883... |
708.2864 | Lattice study of monopoles in the Electroweak theory | We investigated numerically properties of Nambu monopoles in lattice
Electroweak theory at realistic values of $\alpha$ and $\theta_W$. Our choice
of parameters of lattice Lagrangian corresponds to large values of the Higgs
boson mass $M_H > 2 M_W$.
We find that the density of Nambu monopoles cannot be predicted by... | hep-lat hep-ph | we investigated numerically properties of nambu monopoles in lattice electroweak theory at realistic values of alpha and theta_w our choice of parameters of lattice lagrangian corresponds to large values of the higgs boson mass m_h 2 m_w we find that the density of nambu monopoles cannot be predicted by the choice of t... | [['we', 'investigated', 'numerically', 'properties', 'of', 'nambu', 'monopoles', 'in', 'lattice', 'electroweak', 'theory', 'at', 'realistic', 'values', 'of', 'alpha', 'and', 'theta_w', 'our', 'choice', 'of', 'parameters', 'of', 'lattice', 'lagrangian', 'corresponds', 'to', 'large', 'values', 'of', 'the', 'higgs', 'boso... | [-0.13915598408094676, 0.248678857663406, -0.05967221885258632, 0.13267662402922137, -0.06352496253807217, -0.10968492168467492, 0.037293420146940454, 0.3530517344873759, -0.20674807341363763, -0.3157355250910886, 0.04097383466151153, -0.2379693418230501, -0.08070047329660625, 0.10845792163707947, 0.0035897329120592575... |
708.2865 | Lectures on Cosmic Inflation and its Potential Stringy Realizations | These notes present a brief introduction to Hot Big Bang cosmology and Cosmic
Inflation, together with a selection of some recent attempts to embed inflation
into string theory. They provide a partial description of lectures presented in
courses at Dubrovnik in August 2006, at CERN in January 2007 and at Cargese in
A... | hep-th astro-ph gr-qc | these notes present a brief introduction to hot big bang cosmology and cosmic inflation together with a selection of some recent attempts to embed inflation into string theory they provide a partial description of lectures presented in courses at dubrovnik in august 2006 at cern in january 2007 and at cargese in august... | [['these', 'notes', 'present', 'a', 'brief', 'introduction', 'to', 'hot', 'big', 'bang', 'cosmology', 'and', 'cosmic', 'inflation', 'together', 'with', 'a', 'selection', 'of', 'some', 'recent', 'attempts', 'to', 'embed', 'inflation', 'into', 'string', 'theory', 'they', 'provide', 'a', 'partial', 'description', 'of', 'l... | [-0.03943282052771085, 0.18827823842703192, -0.18057603032592637, 0.0891501747738616, -0.12393827101698628, -0.19214987376759426, -0.018677678308449686, 0.32095252302831706, -0.15706235716654057, -0.3987055866530648, 0.1198491645131812, -0.31371684072619693, -0.11080446668302664, 0.14184191247827752, -0.146763094413427... |
708.2866 | Precovers, localizations and stable homotopy | We prove a new localization theorem for stable model categories if the
localizing subcategory is generated by a precovering class in the model
category. We use this to show how one may explicitly realize certain Bousfield
localization functors that arise naturally in the study of relative homological
algebra for grou... | math.CT math.RT | we prove a new localization theorem for stable model categories if the localizing subcategory is generated by a precovering class in the model category we use this to show how one may explicitly realize certain bousfield localization functors that arise naturally in the study of relative homological algebra for group a... | [['we', 'prove', 'a', 'new', 'localization', 'theorem', 'for', 'stable', 'model', 'categories', 'if', 'the', 'localizing', 'subcategory', 'is', 'generated', 'by', 'a', 'precovering', 'class', 'in', 'the', 'model', 'category', 'we', 'use', 'this', 'to', 'show', 'how', 'one', 'may', 'explicitly', 'realize', 'certain', 'b... | [-0.1300797431327987, 0.0493092031820732, -0.0629091477021575, 0.14483423642448934, -0.056243811715759484, -0.17208397070712902, -0.05859760333802186, 0.39539374438954483, -0.46103160828351974, -0.18243826591574094, 0.09611751932614282, -0.16247208321503565, -0.18195778067570692, 0.16768769936307387, -0.238489145632175... |
708.2867 | Nuclear matter in the crust of neutron stars derived from realistic NN
interactions | Properties of inhomogeneous nuclear matter are evaluated within a
relativistic mean field approximation using density dependent coupling
constants. A parameterization for these coupling constants is presented, which
reproduces the properties of the nucleon self-energy obtained in Dirac
Brueckner Hartree Fock calculat... | nucl-th | properties of inhomogeneous nuclear matter are evaluated within a relativistic mean field approximation using density dependent coupling constants a parameterization for these coupling constants is presented which reproduces the properties of the nucleon selfenergy obtained in dirac brueckner hartree fock calculations ... | [['properties', 'of', 'inhomogeneous', 'nuclear', 'matter', 'are', 'evaluated', 'within', 'a', 'relativistic', 'mean', 'field', 'approximation', 'using', 'density', 'dependent', 'coupling', 'constants', 'a', 'parameterization', 'for', 'these', 'coupling', 'constants', 'is', 'presented', 'which', 'reproduces', 'the', 'p... | [-0.11624520050369086, 0.1668894049944356, -0.13752183176789756, 0.12826635069892134, -0.04525114233260901, -0.06956311487629423, 0.009792358959167023, 0.3438394866649091, -0.1846286171357932, -0.25203841882134514, -0.02454781878325267, -0.2606598742428377, -0.06105988523482866, 0.14504143354248286, 0.07957453540467664... |
708.2868 | Reduced Hamiltonian for intersecting shells | The gauge usually adopted for extracting the reduced Hamiltonian of a thin
spherical shell of matter in general relativity, becomes singular when dealing
with two or more intersecting shells. We introduce here a more general class of
gauges which is apt for dealing with intersecting shells. As an application we
give ... | hep-th astro-ph gr-qc | the gauge usually adopted for extracting the reduced hamiltonian of a thin spherical shell of matter in general relativity becomes singular when dealing with two or more intersecting shells we introduce here a more general class of gauges which is apt for dealing with intersecting shells as an application we give the h... | [['the', 'gauge', 'usually', 'adopted', 'for', 'extracting', 'the', 'reduced', 'hamiltonian', 'of', 'a', 'thin', 'spherical', 'shell', 'of', 'matter', 'in', 'general', 'relativity', 'becomes', 'singular', 'when', 'dealing', 'with', 'two', 'or', 'more', 'intersecting', 'shells', 'we', 'introduce', 'here', 'a', 'more', '... | [-0.13585317852197304, 0.11907074569095304, -0.05363806400980268, 0.11335124099582788, -0.02860756206015746, -0.14583811017108106, -0.013488168659664335, 0.36306104982449183, -0.1801798608952335, -0.256180699772778, 0.05718331820264991, -0.2774897474086001, -0.10161100903392903, 0.13982837600633502, -0.0216729760084057... |
708.2869 | Nonlinearity in the dynamics of photoinduced nucleation process | Nonlinear dynamics of photoinduced cooperative phenomena is studied by
numerical calculations on a model of molecular crystals. We found that the
photoinduced nucleation process is triggered only when certain amount of
excitation energy is supplied in a narrow part of the system, i.e., there
exists a smallest cluster... | physics.comp-ph cond-mat.other physics.chem-ph | nonlinear dynamics of photoinduced cooperative phenomena is studied by numerical calculations on a model of molecular crystals we found that the photoinduced nucleation process is triggered only when certain amount of excitation energy is supplied in a narrow part of the system ie there exists a smallest cluster of exc... | [['nonlinear', 'dynamics', 'of', 'photoinduced', 'cooperative', 'phenomena', 'is', 'studied', 'by', 'numerical', 'calculations', 'on', 'a', 'model', 'of', 'molecular', 'crystals', 'we', 'found', 'that', 'the', 'photoinduced', 'nucleation', 'process', 'is', 'triggered', 'only', 'when', 'certain', 'amount', 'of', 'excita... | [-0.1670303610211704, 0.19587330046342685, -0.054991313331993294, 0.014890061808659993, -0.020430430280976, -0.09614312207559124, 0.07154801057185978, 0.3767873158911243, -0.2719545677304268, -0.26787989027798176, 0.034782047045882794, -0.2686843182425946, -0.14256617573555558, 0.1771327382477466, 0.05693741137074539, ... |
708.287 | Electrical response of molecular systems: the power of self-interaction
corrected Kohn-Sham theory | The accurate prediction of electronic response properties of extended
molecular systems has been a challenge for conventional, explicit density
functionals. We demonstrate that a self-interaction correction implemented
rigorously within Kohn-Sham theory via the Optimized Effective Potential (OEP)
yields polarizabilit... | cond-mat.mtrl-sci | the accurate prediction of electronic response properties of extended molecular systems has been a challenge for conventional explicit density functionals we demonstrate that a selfinteraction correction implemented rigorously within kohnsham theory via the optimized effective potential oep yields polarizabilities clos... | [['the', 'accurate', 'prediction', 'of', 'electronic', 'response', 'properties', 'of', 'extended', 'molecular', 'systems', 'has', 'been', 'a', 'challenge', 'for', 'conventional', 'explicit', 'density', 'functionals', 'we', 'demonstrate', 'that', 'a', 'selfinteraction', 'correction', 'implemented', 'rigorously', 'within... | [-0.0828801667896297, 0.008123589623155016, -0.11165628893032783, 0.12268504436889832, 0.007625007705593651, -0.09859676033992207, 0.04880134555137237, 0.4019214242104102, -0.20825829993312558, -0.33520866512800707, 0.01422334507559285, -0.2920310853585375, -0.15990852141244846, 0.1785725203138127, 0.04680032882430224,... |
708.2871 | Sharpness of the Finsler-Hadwiger inequality | In this paper we shall prove a sharpened version of the Finsler-Hadwiger
inequality which is a strong generalization of Weitzenbock inequality. After
that we give another refinement of this inequality and in the final part we
provide some basic applications.
| math.MG math.HO | in this paper we shall prove a sharpened version of the finslerhadwiger inequality which is a strong generalization of weitzenbock inequality after that we give another refinement of this inequality and in the final part we provide some basic applications | [['in', 'this', 'paper', 'we', 'shall', 'prove', 'a', 'sharpened', 'version', 'of', 'the', 'finslerhadwiger', 'inequality', 'which', 'is', 'a', 'strong', 'generalization', 'of', 'weitzenbock', 'inequality', 'after', 'that', 'we', 'give', 'another', 'refinement', 'of', 'this', 'inequality', 'and', 'in', 'the', 'final', ... | [-0.11750038331135726, 0.03377709105515327, -0.15162107687539014, 0.1160597534557709, -0.08085462245612572, -0.13707910088870007, 0.03899819736118214, 0.278350976224129, -0.3070042163897783, -0.24172139191665712, 0.13827475511994308, -0.21108030757078758, -0.21273659747571516, 0.19266710134270865, -0.18160353863659578,... |
708.2872 | Theory of induced quadrupolar order in tetragonal YbRu_{2}Ge_{2} | The tetragonal compound YbRu$_{2}$Ge$_{2}$ exhibits a non-magnetic transition
at $T_0$=10.2K and a magnetic transition at $T_1$=6.5K in zero magnetic field.
We present a model for this material based on a quasi-quartet of Yb$^{3+}$
crystalline electric field (CEF) states and discuss its mean field solution.
Taking in... | cond-mat.str-el cond-mat.mtrl-sci | the tetragonal compound ybru_2ge_2 exhibits a nonmagnetic transition at t_0102k and a magnetic transition at t_165k in zero magnetic field we present a model for this material based on a quasiquartet of yb3 crystalline electric field cef states and discuss its mean field solution taking into account the broadening of t... | [['the', 'tetragonal', 'compound', 'ybru_2ge_2', 'exhibits', 'a', 'nonmagnetic', 'transition', 'at', 't_0102k', 'and', 'a', 'magnetic', 'transition', 'at', 't_165k', 'in', 'zero', 'magnetic', 'field', 'we', 'present', 'a', 'model', 'for', 'this', 'material', 'based', 'on', 'a', 'quasiquartet', 'of', 'yb3', 'crystalline... | [-0.19643136090790894, 0.22416827825133454, 0.006266786762932827, 0.03210812947037374, -0.06390216568571894, -0.11862163390749349, 0.046928376744240316, 0.39075950487097216, -0.25142773986886163, -0.31358372543907753, 0.0023807480587153236, -0.2723027071403851, -0.03447148475698758, 0.1404109769884579, 0.08076318526374... |
708.2873 | Global lopsided instability in a purely stellar galactic disc | It is shown that pure exponential discs in spiral galaxies are capable of
supporting slowly varying discrete global lopsided modes, which can explain the
observed features of lopsidedness in the stellar discs. Using linearized fluid
dynamical equations with the softened self-gravity and pressure of the
perturbation a... | astro-ph | it is shown that pure exponential discs in spiral galaxies are capable of supporting slowly varying discrete global lopsided modes which can explain the observed features of lopsidedness in the stellar discs using linearized fluid dynamical equations with the softened selfgravity and pressure of the perturbation as the... | [['it', 'is', 'shown', 'that', 'pure', 'exponential', 'discs', 'in', 'spiral', 'galaxies', 'are', 'capable', 'of', 'supporting', 'slowly', 'varying', 'discrete', 'global', 'lopsided', 'modes', 'which', 'can', 'explain', 'the', 'observed', 'features', 'of', 'lopsidedness', 'in', 'the', 'stellar', 'discs', 'using', 'line... | [-0.1640943533834275, 0.14899839673576967, -0.09123931250161602, 0.0927243116311729, -0.06665386827375396, -0.056578982480399574, -0.010212862388218552, 0.3219079346433723, -0.26657196588810156, -0.2733546526946685, 0.06080573664656081, -0.2403124137022553, -0.08710693239053867, 0.18302350311790336, 0.00070157853500827... |
708.2874 | Search for the Rare Decay K_{L}\to\pi^{0}\pi^{0}\gamma | The KTeV E799 experiment has conducted a search for the rare decay
$K_{L}\to\pi^{0}\pi^{0}\gamma$ via the topology
$K_{L}\to\pi^{0}\pi^{0}_D\gamma$ (where $\pi^0_D\to\gamma e^+e^-$). Due to Bose
statistics of the $\pi^0$ pair and the real nature of the photon, the
$K_{L}\to\pi^{0}\pi^{0}\gamma$ decay is restricted to... | hep-ex | the ktev e799 experiment has conducted a search for the rare decay k_ltopi0pi0gamma via the topology k_ltopi0pi0_dgamma where pi0_dtogamma ee due to bose statistics of the pi0 pair and the real nature of the photon the k_ltopi0pi0gamma decay is restricted to proceed at lowest order by the cp conserving direct emission ... | [['the', 'ktev', 'e799', 'experiment', 'has', 'conducted', 'a', 'search', 'for', 'the', 'rare', 'decay', 'k_ltopi0pi0gamma', 'via', 'the', 'topology', 'k_ltopi0pi0_dgamma', 'where', 'pi0_dtogamma', 'ee', 'due', 'to', 'bose', 'statistics', 'of', 'the', 'pi0', 'pair', 'and', 'the', 'real', 'nature', 'of', 'the', 'photon'... | [-0.13390875990520917, 0.1973619683251998, -0.05758363148197532, 0.0645253925238872, -0.020104516810214704, -0.08495314880846101, 0.10950112387664583, 0.26644993783383253, -0.17766134959968263, -0.27800534796296505, 0.026860462678310444, -0.32047752789711875, -0.04989826985585846, 0.13989249843769103, 0.084073374533960... |
708.2875 | Surfing on the Edge: Chaos vs. Near-Integrability in the System of
Jovian Planets | We demonstrate that the system of Jovian planets
(Sun+Jupiter+Saturn+Uranus+Neptune), integrated for 200 million years as an
isolated 5-body system using many sets of initial conditions all within the
uncertainty bounds of their currently known positions, can display both chaos
and near-integrability. The conclusion ... | astro-ph | we demonstrate that the system of jovian planets sunjupitersaturnuranusneptune integrated for 200 million years as an isolated 5body system using many sets of initial conditions all within the uncertainty bounds of their currently known positions can display both chaos and nearintegrability the conclusion is consistent... | [['we', 'demonstrate', 'that', 'the', 'system', 'of', 'jovian', 'planets', 'sunjupitersaturnuranusneptune', 'integrated', 'for', '200', 'million', 'years', 'as', 'an', 'isolated', '5body', 'system', 'using', 'many', 'sets', 'of', 'initial', 'conditions', 'all', 'within', 'the', 'uncertainty', 'bounds', 'of', 'their', '... | [-0.14058117838035936, 0.09090577056974455, -0.08605147611482868, 0.06590799799554849, -0.012618548481259494, -0.10836782111852829, 0.04706820403392028, 0.36836669464994753, -0.20307781489141885, -0.36716065578096146, 0.12071035023296385, -0.26015444260888865, -0.0784168956992549, 0.2691126708806093, -0.055124227093204... |
708.2876 | Tkachenko modes as sources of quasiperiodic pulsar spin variations | We study the long wavelength shear modes (Tkachenko waves) of triangular
lattices of singly quantized vortices in neutron star interiors taking into
account the mutual friction between the superfluid and the normal fluid and the
shear viscosity of the normal fluid. The set of Tkachenko modes that propagate
in the pla... | astro-ph nucl-th | we study the long wavelength shear modes tkachenko waves of triangular lattices of singly quantized vortices in neutron star interiors taking into account the mutual friction between the superfluid and the normal fluid and the shear viscosity of the normal fluid the set of tkachenko modes that propagate in the plane or... | [['we', 'study', 'the', 'long', 'wavelength', 'shear', 'modes', 'tkachenko', 'waves', 'of', 'triangular', 'lattices', 'of', 'singly', 'quantized', 'vortices', 'in', 'neutron', 'star', 'interiors', 'taking', 'into', 'account', 'the', 'mutual', 'friction', 'between', 'the', 'superfluid', 'and', 'the', 'normal', 'fluid', ... | [-0.24167209231250342, 0.3342925447527142, -0.035252639837563035, 0.015987938186819, -0.09427443710821015, -0.0987638438031787, -0.0016372150342379298, 0.319293256050774, -0.2785102187788912, -0.22617028592420477, 0.05045803470004882, -0.29064948851647343, -0.04705475110205866, 0.18913994257648786, 0.04158269747027329,... |
708.2877 | The mid-infrared emission of Seyfert galaxies. A new analysis of ISOCAM
data | We present mid-infrared data of a sample of 57 AGNs obtained with the
instrument ISOCAM on board the satellite ISO. The images were obtained through
the LW2 (6.75 microns) and LW7 (9.62 microns) filters. This is a new analysis
of Clavel et al. (2000) galaxy sample, which is divided into 26 type 1 (< or =
1.5) and 28 ... | astro-ph | we present midinfrared data of a sample of 57 agns obtained with the instrument isocam on board the satellite iso the images were obtained through the lw2 675 microns and lw7 962 microns filters this is a new analysis of clavel et al 2000 galaxy sample which is divided into 26 type 1 or 15 and 28 type 2 15 seyfert gala... | [['we', 'present', 'midinfrared', 'data', 'of', 'a', 'sample', 'of', '57', 'agns', 'obtained', 'with', 'the', 'instrument', 'isocam', 'on', 'board', 'the', 'satellite', 'iso', 'the', 'images', 'were', 'obtained', 'through', 'the', 'lw2', '675', 'microns', 'and', 'lw7', '962', 'microns', 'filters', 'this', 'is', 'a', 'n... | [-0.02988510753980664, 0.06747757230596281, -0.0667119240618449, 0.09869409112273911, -0.05378973449690147, -0.08369897257982835, 0.009661124506611165, 0.4479674348437684, -0.1589538693669723, -0.3330987421052084, 0.06622484089680965, -0.310952087129491, -0.014408251839891755, 0.1747360149506451, -0.019152924765482148,... |
708.2878 | Noise thermometry and electron thermometry of a sample-on-cantilever
system below 1 Kelvin | We have used two types of thermometry to study thermal fluctuations in a
microcantilever-based system below 1 K. We measured the temperature of a
cantilever's macroscopic degree-of-freedom (via the Brownian motion of its
lowest flexural mode) and its microscopic degrees-of-freedom (via the electron
temperature of a m... | cond-mat.other | we have used two types of thermometry to study thermal fluctuations in a microcantileverbased system below 1 k we measured the temperature of a cantilevers macroscopic degreeoffreedom via the brownian motion of its lowest flexural mode and its microscopic degreesoffreedom via the electron temperature of a metal sample ... | [['we', 'have', 'used', 'two', 'types', 'of', 'thermometry', 'to', 'study', 'thermal', 'fluctuations', 'in', 'a', 'microcantileverbased', 'system', 'below', '1', 'k', 'we', 'measured', 'the', 'temperature', 'of', 'a', 'cantilevers', 'macroscopic', 'degreeoffreedom', 'via', 'the', 'brownian', 'motion', 'of', 'its', 'low... | [-0.11761919221811995, 0.2154502397662355, -0.0794410377923284, -0.024332233616414952, -0.02342837890514086, -0.1681456529996214, 0.10411773445132698, 0.4010772052576247, -0.25138758760444896, -0.31876982481593324, 0.07351194467928414, -0.3402359883886637, -0.04929274465101435, 0.2540086228016418, 0.044885318236636745,... |
708.2879 | On Shannon-Jaynes Entropy and Fisher Information | The fundamentals of the Maximum Entropy principle as a rule for assigning and
updating probabilities are revisited. The Shannon-Jaynes relative entropy is
vindicated as the optimal criterion for use with an updating rule. A
constructive rule is justified which assigns the probabilities least sensitive
to coarse-grain... | physics.data-an physics.gen-ph | the fundamentals of the maximum entropy principle as a rule for assigning and updating probabilities are revisited the shannonjaynes relative entropy is vindicated as the optimal criterion for use with an updating rule a constructive rule is justified which assigns the probabilities least sensitive to coarsegraining th... | [['the', 'fundamentals', 'of', 'the', 'maximum', 'entropy', 'principle', 'as', 'a', 'rule', 'for', 'assigning', 'and', 'updating', 'probabilities', 'are', 'revisited', 'the', 'shannonjaynes', 'relative', 'entropy', 'is', 'vindicated', 'as', 'the', 'optimal', 'criterion', 'for', 'use', 'with', 'an', 'updating', 'rule', ... | [-0.05107728505390696, 0.12524453867285956, -0.10523443380952813, 0.1601910219869751, -0.12070988705090713, -0.1823975414808956, 0.18019478520363919, 0.3231242662295699, -0.2682486890407745, -0.2539823426050134, 0.1598964175209403, -0.22696166722744238, -0.1167722053514808, 0.14676241619235952, -0.06198475849305396, 0.... |
708.288 | Entanglement of superconducting charge qubits by homodyne measurement | We present a scheme by which projective homodyne measurement of a microwave
resonator can be used to generate entanglement between two superconducting
charge qubits coupled to this resonator. The non-interacting qubits are
initialised in a product of their ground states, the resonator is initialised
in a coherent fie... | quant-ph cond-mat.supr-con | we present a scheme by which projective homodyne measurement of a microwave resonator can be used to generate entanglement between two superconducting charge qubits coupled to this resonator the noninteracting qubits are initialised in a product of their ground states the resonator is initialised in a coherent field st... | [['we', 'present', 'a', 'scheme', 'by', 'which', 'projective', 'homodyne', 'measurement', 'of', 'a', 'microwave', 'resonator', 'can', 'be', 'used', 'to', 'generate', 'entanglement', 'between', 'two', 'superconducting', 'charge', 'qubits', 'coupled', 'to', 'this', 'resonator', 'the', 'noninteracting', 'qubits', 'are', '... | [-0.19112517202152152, 0.23194130578796818, -0.07546996546354685, -0.002520721507941209, 0.01771999554324696, -0.21090219003141267, 0.05984962947545786, 0.37827788970881066, -0.20234338946343677, -0.2648675401574214, 0.04572126689146607, -0.27269612916012986, -0.033207416571747826, 0.2423761906599953, -0.01103585906327... |
708.2881 | Spin-polarized tunneling currents through a ferromagnetic insulator
between two metallic or superconducting leads | Using the Keldysh formalism the tunneling current through a hybrid structure
where a confined magnetic insulator (I) is sandwiched between two non-magnetic
leads is calculated. The leads can be either normal metals (M) or
superconductors (S). Each region is modelled as a single band in tight-binding
approximation in ... | cond-mat.str-el | using the keldysh formalism the tunneling current through a hybrid structure where a confined magnetic insulator i is sandwiched between two nonmagnetic leads is calculated the leads can be either normal metals m or superconductors s each region is modelled as a single band in tightbinding approximation in order to und... | [['using', 'the', 'keldysh', 'formalism', 'the', 'tunneling', 'current', 'through', 'a', 'hybrid', 'structure', 'where', 'a', 'confined', 'magnetic', 'insulator', 'i', 'is', 'sandwiched', 'between', 'two', 'nonmagnetic', 'leads', 'is', 'calculated', 'the', 'leads', 'can', 'be', 'either', 'normal', 'metals', 'm', 'or', ... | [-0.14994180699087387, 0.15680384062129873, -0.0621788783525852, 0.08587334831354622, -0.007935885336911795, -0.1827455969637652, 0.07551749155467596, 0.37625925692172085, -0.25407602982656835, -0.2889716522032885, -0.022031943119241316, -0.32000186947468473, -0.1137657952831911, 0.14676205257848396, 0.0472176306784125... |
708.2882 | Phase field model of interfaces in single-component systems derived from
classical density functional theory | Phase field models have been applied in recent years to grain boundaries in
single-component systems. The models are based on the minimization of a free
energy functional, which is constructed phenomenologically rather than being
derived from first principles. In single-component systems the free energy is a
function... | cond-mat.mtrl-sci cond-mat.stat-mech | phase field models have been applied in recent years to grain boundaries in singlecomponent systems the models are based on the minimization of a free energy functional which is constructed phenomenologically rather than being derived from first principles in singlecomponent systems the free energy is a functional of a... | [['phase', 'field', 'models', 'have', 'been', 'applied', 'in', 'recent', 'years', 'to', 'grain', 'boundaries', 'in', 'singlecomponent', 'systems', 'the', 'models', 'are', 'based', 'on', 'the', 'minimization', 'of', 'a', 'free', 'energy', 'functional', 'which', 'is', 'constructed', 'phenomenologically', 'rather', 'than'... | [-0.09259661801840778, 0.12888101488769044, -0.1582354214302935, 0.06408060478759682, -0.0651993278440062, -0.09163962211134238, 0.05221385469210783, 0.35334946968026093, -0.24383077953296545, -0.32935413363278954, 0.10700118465274182, -0.22504042420484177, -0.17205422946050034, 0.18540501119601507, -0.0477068919909896... |
708.2883 | Positive bases in spaces of polynomials | For a nonempty compact set D of R we determine the maximal possible dimension
of a subspace X of polynomial functions of degree at most m which possesses a
positive bases (where positivity is understood on D). The exact value of this
maximal dimension depends on topological features of the base set D. We show
that at... | math.CA math.FA | for a nonempty compact set d of r we determine the maximal possible dimension of a subspace x of polynomial functions of degree at most m which possesses a positive bases where positivity is understood on d the exact value of this maximal dimension depends on topological features of the base set d we show that at many ... | [['for', 'a', 'nonempty', 'compact', 'set', 'd', 'of', 'r', 'we', 'determine', 'the', 'maximal', 'possible', 'dimension', 'of', 'a', 'subspace', 'x', 'of', 'polynomial', 'functions', 'of', 'degree', 'at', 'most', 'm', 'which', 'possesses', 'a', 'positive', 'bases', 'where', 'positivity', 'is', 'understood', 'on', 'd', ... | [-0.1940694628652954, 0.1097951526236203, -0.03310413990494988, -0.005489943092615004, -0.03301195221738742, -0.17199142847860616, 0.03095429730675523, 0.32347627310082316, -0.254202360940528, -0.21671122954493122, 0.09276164098668636, -0.26955914175108314, -0.10693243403534686, 0.1913161908183062, 0.001081788735020728... |
708.2884 | Mid-Infrared interferometry of dust around massive evolved stars | We report long-baseline interferometric measurements of circumstellar dust
around massive evolved stars with the MIDI instrument on the Very Large
Telescope Interferometer and provide spectrally dispersed visibilities in the
8-13 micron wavelength band. We also present diffraction-limited observations
at 10.7 micron ... | astro-ph | we report longbaseline interferometric measurements of circumstellar dust around massive evolved stars with the midi instrument on the very large telescope interferometer and provide spectrally dispersed visibilities in the 813 micron wavelength band we also present diffractionlimited observations at 107 micron on the ... | [['we', 'report', 'longbaseline', 'interferometric', 'measurements', 'of', 'circumstellar', 'dust', 'around', 'massive', 'evolved', 'stars', 'with', 'the', 'midi', 'instrument', 'on', 'the', 'very', 'large', 'telescope', 'interferometer', 'and', 'provide', 'spectrally', 'dispersed', 'visibilities', 'in', 'the', '813', ... | [-0.05031225864025815, 0.10659040962499412, -0.05745312909428508, 0.048309213415107216, -0.07412324914104909, -0.10097932323409183, 0.06277084867674652, 0.44461651469816216, -0.14634589262088357, -0.3358571898335448, 0.056666864426346025, -0.28491992204903793, -0.020353677308173244, 0.13946247227958114, -0.068815720181... |
708.2885 | Measurement of B -> D_s K pi branching ratios | We report a measurement of the exclusive $B^+$ meson decay to the final state
$D_s^- K^+\pi^+$ using $520 \times 10^{6} B\bar{B}$ pairs collected near the
$\Upsilon(4S)$ resonance, with the Belle detector at the KEKB asymmetric-energy
$e^+e^-$ collider. Using the $D_S^- \to \phi \pi^-$ decay mode to reconstruct
$D_s^... | hep-ex | we report a measurement of the exclusive b meson decay to the final state d_s kpi using 520 times 106 bbarb pairs collected near the upsilon4s resonance with the belle detector at the kekb asymmetricenergy ee collider using the d_s to phi pi decay mode to reconstruct d_s mesons we obtain the branching fraction cal bbto... | [['we', 'report', 'a', 'measurement', 'of', 'the', 'exclusive', 'b', 'meson', 'decay', 'to', 'the', 'final', 'state', 'd_s', 'kpi', 'using', '520', 'times', '106', 'bbarb', 'pairs', 'collected', 'near', 'the', 'upsilon4s', 'resonance', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetricenergy', 'ee', '... | [-0.12916326015692903, 0.2215990576078184, -0.09306501610924235, 0.040059279823749835, 0.021779383246956222, -0.13369281972038813, 0.0960468435025012, 0.23667923125057397, -0.1284370255783539, -0.2087794657881287, -0.07031250474260146, -0.4837140203876929, 0.11111044029662893, 0.08891909140088088, 0.0875283859323562, 0... |
708.2886 | Polynomial Structure of the (Open) Topological String Partition Function | In this paper we show that the polynomial structure of the topological string
partition function found by Yamaguchi and Yau for the quintic holds for an
arbitrary Calabi-Yau manifold with any number of moduli. Furthermore, we
generalize these results to the open topological string partition function as
discussed rece... | hep-th | in this paper we show that the polynomial structure of the topological string partition function found by yamaguchi and yau for the quintic holds for an arbitrary calabiyau manifold with any number of moduli furthermore we generalize these results to the open topological string partition function as discussed recently ... | [['in', 'this', 'paper', 'we', 'show', 'that', 'the', 'polynomial', 'structure', 'of', 'the', 'topological', 'string', 'partition', 'function', 'found', 'by', 'yamaguchi', 'and', 'yau', 'for', 'the', 'quintic', 'holds', 'for', 'an', 'arbitrary', 'calabiyau', 'manifold', 'with', 'any', 'number', 'of', 'moduli', 'further... | [-0.13234362482898315, 0.06364612197883278, -0.0503880628779278, 0.11104495749982485, -0.07805785650418977, -0.12713060097105927, -0.008410554787664974, 0.28964877153857277, -0.2344404201702041, -0.2851242770567157, 0.06672334969951377, -0.23509277509115004, -0.2633286795685693, 0.2139307053728124, -0.0996123021942074,... |
708.2887 | Bordered Riemann surfaces in C^2 | One of the oldest open problems in the classical function theory is whether
every open Riemann surface admits a proper holomorphic embedding into C^2. In
this paper we prove the following Theorem: If D is a bordered Riemann surface
whose closure admits an injective immersion in C^2 that is holomorphic in D,
then D ad... | math.CV math.AG | one of the oldest open problems in the classical function theory is whether every open riemann surface admits a proper holomorphic embedding into c2 in this paper we prove the following theorem if d is a bordered riemann surface whose closure admits an injective immersion in c2 that is holomorphic in d then d admits a ... | [['one', 'of', 'the', 'oldest', 'open', 'problems', 'in', 'the', 'classical', 'function', 'theory', 'is', 'whether', 'every', 'open', 'riemann', 'surface', 'admits', 'a', 'proper', 'holomorphic', 'embedding', 'into', 'c2', 'in', 'this', 'paper', 'we', 'prove', 'the', 'following', 'theorem', 'if', 'd', 'is', 'a', 'borde... | [-0.13536764878091645, 0.06643695550208266, -0.10568970067611148, 0.034183826331082766, -0.11511699557786824, -0.16260464261663524, 0.01004101156345191, 0.33128259389719983, -0.2750090595464818, -0.24130661106827828, 0.07545335223764046, -0.24358703797160824, -0.1863280559920387, 0.18325180409325137, -0.157082837771389... |
708.2888 | Another look at the problem of gauge invariance in QFT | It is generally assumed that quantum field theory (QFT) is gauge invariant.
However it is well known that non-gauge invariant terms appear in various
calculations. This problem was examined in Refs. [3] and [4] and it was shown
that at the formal level QFT in the Schroedinger picture is not, in fact, gauge
invariant.... | quant-ph | it is generally assumed that quantum field theory qft is gauge invariant however it is well known that nongauge invariant terms appear in various calculations this problem was examined in refs 3 and 4 and it was shown that at the formal level qft in the schroedinger picture is not in fact gauge invariant it was determi... | [['it', 'is', 'generally', 'assumed', 'that', 'quantum', 'field', 'theory', 'qft', 'is', 'gauge', 'invariant', 'however', 'it', 'is', 'well', 'known', 'that', 'nongauge', 'invariant', 'terms', 'appear', 'in', 'various', 'calculations', 'this', 'problem', 'was', 'examined', 'in', 'refs', '3', 'and', '4', 'and', 'it', 'w... | [-0.10515666386267791, 0.15590369037042062, -0.1295878627182295, 0.11610686998193463, -0.08847494788467884, -0.13399027054508528, -0.028604408903047444, 0.3455369513606032, -0.24903392650187015, -0.3021051556741198, 0.06868384789209812, -0.231290531787187, -0.18462136208390195, 0.1571241393685341, -0.0934891734023889, ... |
708.2889 | Probing quantum gravity using photons from a flare of the active
galactic nucleus Markarian 501 observed by the MAGIC telescope | We analyze the timing of photons observed by the MAGIC telescope during a
flare of the active galactic nucleus Mkn 501 for a possible correlation with
energy, as suggested by some models of quantum gravity (QG), which predict a
vacuum refractive index \simeq 1 + (E/M_{QGn})^n, n = 1,2. Parametrizing the
delay between... | astro-ph gr-qc hep-ph hep-th | we analyze the timing of photons observed by the magic telescope during a flare of the active galactic nucleus mkn 501 for a possible correlation with energy as suggested by some models of quantum gravity qg which predict a vacuum refractive index simeq 1 em_qgnn n 12 parametrizing the delay between gammarays of differ... | [['we', 'analyze', 'the', 'timing', 'of', 'photons', 'observed', 'by', 'the', 'magic', 'telescope', 'during', 'a', 'flare', 'of', 'the', 'active', 'galactic', 'nucleus', 'mkn', '501', 'for', 'a', 'possible', 'correlation', 'with', 'energy', 'as', 'suggested', 'by', 'some', 'models', 'of', 'quantum', 'gravity', 'qg', 'w... | [-0.09239510220217229, 0.2252213761969587, -0.021324744745462882, 0.1497407786102042, -0.020551962950149504, -0.13927303737874666, 0.08596712286474512, 0.4046313473563485, -0.18643361226334668, -0.40697359104304254, 0.026700367838997364, -0.31485224402501805, -0.004301171863310728, 0.2016772844754316, 0.040945599779111... |
708.289 | Linear maps preserving invariants | Let $G\subset\GL(V)$ be a complex reductive group. Let $G'$ denote
$\{\phi\in\GL(V)\mid p\circ\phi=p\text{for all} p\in\C[V]^G\}$. We show that,
in general, $G'=G$. In case $G$ is the adjoint group of a simple Lie algebra
$\lieg$, we show that $G'$ is an order 2 extension of $G$. We also calculate
$G'$ for all repres... | math.RT math.GR | let gsubsetglv be a complex reductive group let g denote phiinglvmid pcircphiptextfor all pincvg we show that in general gg in case g is the adjoint group of a simple lie algebra lieg we show that g is an order 2 extension of g we also calculate g for all representations of sl_2 | [['let', 'gsubsetglv', 'be', 'a', 'complex', 'reductive', 'group', 'let', 'g', 'denote', 'phiinglvmid', 'pcircphiptextfor', 'all', 'pincvg', 'we', 'show', 'that', 'in', 'general', 'gg', 'in', 'case', 'g', 'is', 'the', 'adjoint', 'group', 'of', 'a', 'simple', 'lie', 'algebra', 'lieg', 'we', 'show', 'that', 'g', 'is', 'a... | [-0.24108744028490037, 0.11980812815279933, -0.10584807712584735, -0.026475178259424866, -0.19694023756310344, -0.09855811892077326, -0.07192346878349781, 0.40320567712187766, -0.3103536782413721, -0.20323900658637284, 0.04536031965631992, -0.241407051384449, -0.15340932415798306, 0.20841040082275866, -0.11234408225398... |
708.2891 | Magnons in Ferromagnetic Metallic Manganites | Ferromagnetic (FM) manganites, a group of likely half-metallic oxides, are of
special interest not only because they are a testing ground of the classical
doubleexchange interaction mechanism for the colossal magnetoresistance, but
also because they exhibit an extraordinary arena of emergent phenomena. These
emergent... | cond-mat.str-el cond-mat.mtrl-sci | ferromagnetic fm manganites a group of likely halfmetallic oxides are of special interest not only because they are a testing ground of the classical doubleexchange interaction mechanism for the colossal magnetoresistance but also because they exhibit an extraordinary arena of emergent phenomena these emergent phenomen... | [['ferromagnetic', 'fm', 'manganites', 'a', 'group', 'of', 'likely', 'halfmetallic', 'oxides', 'are', 'of', 'special', 'interest', 'not', 'only', 'because', 'they', 'are', 'a', 'testing', 'ground', 'of', 'the', 'classical', 'doubleexchange', 'interaction', 'mechanism', 'for', 'the', 'colossal', 'magnetoresistance', 'bu... | [-0.2235996419247905, 0.24207845004036374, -0.010110135762287038, 0.0894578780563149, -0.10526258854827444, -0.13094552054868214, 0.08067933144879394, 0.39635189965899503, -0.2769572711150561, -0.2509457909202735, 0.027385299733058283, -0.3430260040747401, -0.17124261338529842, 0.15571685109087932, 0.04484957663142788,... |
708.2892 | Comparison of hybrid and pure Monte Carlo shower generators on an event
by event basis | SENECA is a hybrid air shower simulation written by H. Drescher that utilizes
both Monte Carlo simulation and cascade equations. By using the cascade
equations only in the high energy portion of the shower, where the shower is
inherently one-dimensional, SENECA is able to utilize the advantages in speed
from the casc... | astro-ph | seneca is a hybrid air shower simulation written by h drescher that utilizes both monte carlo simulation and cascade equations by using the cascade equations only in the high energy portion of the shower where the shower is inherently onedimensional seneca is able to utilize the advantages in speed from the cascade equ... | [['seneca', 'is', 'a', 'hybrid', 'air', 'shower', 'simulation', 'written', 'by', 'h', 'drescher', 'that', 'utilizes', 'both', 'monte', 'carlo', 'simulation', 'and', 'cascade', 'equations', 'by', 'using', 'the', 'cascade', 'equations', 'only', 'in', 'the', 'high', 'energy', 'portion', 'of', 'the', 'shower', 'where', 'th... | [-0.021150495351987406, 0.2134607755585203, -0.07399142211431008, 0.12460489908767265, 0.022328416615759544, -0.031055411196558653, -0.06664237383197766, 0.42270671030585194, -0.19918150228706183, -0.4118443280450252, 0.02200376884869689, -0.32752683885754064, 0.008052720635814565, 0.18726315461820595, 0.05266925977529... |
708.2893 | Fast Recursive Coding Based on Grouping of Symbols | A novel fast recursive coding technique is proposed. It operates with only
integer values not longer 8 bits and is multiplication free. Recursion the
algorithm is based on indirectly provides rather effective coding of symbols
for very large alphabets. The code length for the proposed technique can be up
to 20-30% le... | cs.IT math.IT | a novel fast recursive coding technique is proposed it operates with only integer values not longer 8 bits and is multiplication free recursion the algorithm is based on indirectly provides rather effective coding of symbols for very large alphabets the code length for the proposed technique can be up to 2030 less than... | [['a', 'novel', 'fast', 'recursive', 'coding', 'technique', 'is', 'proposed', 'it', 'operates', 'with', 'only', 'integer', 'values', 'not', 'longer', '8', 'bits', 'and', 'is', 'multiplication', 'free', 'recursion', 'the', 'algorithm', 'is', 'based', 'on', 'indirectly', 'provides', 'rather', 'effective', 'coding', 'of',... | [-0.14143208394855705, 0.14716876237027682, -0.07027009132999315, 0.11157502597215266, -0.08176860165149807, -0.2675453305675356, 0.0874568190488186, 0.37896807201262284, -0.2680712163920945, -0.32655658328266285, 0.1419722732319844, -0.20875191993280764, -0.14364172262487127, 0.28630565340394404, -0.09427133235218588,... |
708.2894 | On the growth of the Bergman kernel near an infinite-type point | We study diagonal estimates for the Bergman kernels of certain model domains
in $\mathbb{C}^2$ near boundary points that are of infinite type. To do so, we
need a mild structural condition on the defining functions of interest that
facilitates optimal upper and lower bounds. This is a mild condition; unlike
earlier s... | math.CV | we study diagonal estimates for the bergman kernels of certain model domains in mathbbc2 near boundary points that are of infinite type to do so we need a mild structural condition on the defining functions of interest that facilitates optimal upper and lower bounds this is a mild condition unlike earlier studies of th... | [['we', 'study', 'diagonal', 'estimates', 'for', 'the', 'bergman', 'kernels', 'of', 'certain', 'model', 'domains', 'in', 'mathbbc2', 'near', 'boundary', 'points', 'that', 'are', 'of', 'infinite', 'type', 'to', 'do', 'so', 'we', 'need', 'a', 'mild', 'structural', 'condition', 'on', 'the', 'defining', 'functions', 'of', ... | [-0.1439544049082933, 0.08739130048064415, -0.0775116023424769, 0.08875024830269689, -0.10746219769886164, -0.1414953469664346, 0.05451716330537799, 0.3996769659934896, -0.25939620895502724, -0.23117723206937243, 0.15044689106768014, -0.23786966512240817, -0.14312868145790614, 0.21467802969294938, -0.14274758251087966,... |
708.2895 | Random Matrices: The circular Law | Let $\a$ be a complex random variable with mean zero and bounded variance
$\sigma^{2}$. Let $N_{n}$ be a random matrix of order $n$ with entries being
i.i.d. copies of $\a$. Let $\lambda_{1}, ..., \lambda_{n}$ be the eigenvalues
of $\frac{1}{\sigma \sqrt n}N_{n}$. Define the empirical spectral distribution
$\mu_{n}$ ... | math.PR math.SP | let a be a complex random variable with mean zero and bounded variance sigma2 let n_n be a random matrix of order n with entries being iid copies of a let lambda_1 lambda_n be the eigenvalues of frac1sigma sqrt nn_n define the empirical spectral distribution mu_n of n_n by the formula mu_nst frac1n k leq n relambda_k l... | [['let', 'a', 'be', 'a', 'complex', 'random', 'variable', 'with', 'mean', 'zero', 'and', 'bounded', 'variance', 'sigma2', 'let', 'n_n', 'be', 'a', 'random', 'matrix', 'of', 'order', 'n', 'with', 'entries', 'being', 'iid', 'copies', 'of', 'a', 'let', 'lambda_1', 'lambda_n', 'be', 'the', 'eigenvalues', 'of', 'frac1sigma'... | [-0.1254533975286929, 0.18483701912800268, -0.09870420001624595, -0.011841781629838658, -0.013745260250684963, -0.18716656147394659, 0.039346598779313825, 0.2886102026214405, -0.26556031234549726, -0.22526469345990138, 0.07445158241047416, -0.3118654370345936, -0.10735119781916214, 0.1448891675764961, -0.09331135538590... |
708.2896 | Approximating a Wavefunction as an Unconstrained Sum of Slater
Determinants | The wavefunction for the multiparticle Schr\"odinger equation is a function
of many variables and satisfies an antisymmetry condition, so it is natural to
approximate it as a sum of Slater determinants. Many current methods do so, but
they impose additional structural constraints on the determinants, such as
orthogon... | math-ph math.MP math.NA physics.chem-ph | the wavefunction for the multiparticle schrodinger equation is a function of many variables and satisfies an antisymmetry condition so it is natural to approximate it as a sum of slater determinants many current methods do so but they impose additional structural constraints on the determinants such as orthogonality be... | [['the', 'wavefunction', 'for', 'the', 'multiparticle', 'schrodinger', 'equation', 'is', 'a', 'function', 'of', 'many', 'variables', 'and', 'satisfies', 'an', 'antisymmetry', 'condition', 'so', 'it', 'is', 'natural', 'to', 'approximate', 'it', 'as', 'a', 'sum', 'of', 'slater', 'determinants', 'many', 'current', 'method... | [-0.1097221577049784, 0.029801916714219057, -0.1256486215353222, 0.09342880473098338, -0.1011007742474223, -0.10951677967571247, 0.04978676930784812, 0.35989943358384757, -0.30216455235290274, -0.30171907649860835, 0.10989984881762467, -0.2482553217756811, -0.18894674145603474, 0.17034328253333075, -0.00312884121110111... |
708.2897 | Diagrammatic bounds on the lace-expansion coefficients for oriented
percolation | We provide a complete proof of the diagrammatic bounds on the lace-expansion
coefficients for oriented percolation, which are used in [arXiv:math/0703455]
to investigate critical behavior for long-range oriented percolation above
2\min{\alpha,2} spatial dimensions.
| math.PR math-ph math.MP | we provide a complete proof of the diagrammatic bounds on the laceexpansion coefficients for oriented percolation which are used in arxivmath0703455 to investigate critical behavior for longrange oriented percolation above 2minalpha2 spatial dimensions | [['we', 'provide', 'a', 'complete', 'proof', 'of', 'the', 'diagrammatic', 'bounds', 'on', 'the', 'laceexpansion', 'coefficients', 'for', 'oriented', 'percolation', 'which', 'are', 'used', 'in', 'arxivmath0703455', 'to', 'investigate', 'critical', 'behavior', 'for', 'longrange', 'oriented', 'percolation', 'above', '2min... | [-0.12627926285588933, 0.15003553432442487, -0.07424226469330249, 0.10370872337971965, -0.059953951877692056, -0.1280279941406221, 0.031096922984767343, 0.399057706157046, -0.17612588303464075, -0.20689052379419726, 0.07471981007350428, -0.2617281160407489, -0.15136181445972574, 0.16090605558166582, 0.005861374880037, ... |
708.2898 | On solutions to Walcher's extended holomorphic anomaly equation | We give a generalization of Yamaguchi--Yau's result to Walcher's extended
holomorphic anomaly equation.
| math.AG hep-th | we give a generalization of yamaguchiyaus result to walchers extended holomorphic anomaly equation | [['we', 'give', 'a', 'generalization', 'of', 'yamaguchiyaus', 'result', 'to', 'walchers', 'extended', 'holomorphic', 'anomaly', 'equation']] | [-0.20288279031713805, -0.07638864940963686, -0.16260199030997077, 0.13510188149909177, -0.21801077403749028, -0.14420377381611615, 0.03415806560466687, 0.2210224655767282, -0.25072626769542694, -0.27642376938213903, 0.05173820625835409, -0.2282113420466582, -0.2593954318823914, 0.14763625307629505, -0.1249070106229434... |
708.2899 | A rigidity theorem for holomorphic generators on the Hilbert ball | We present a rigidity property of holomorphic generators on the open unit
ball $\mathbb{B}$ of a Hilbert space $H$. Namely, if $f\in\Hol (\mathbb{B},H)$
is the generator of a one-parameter continuous semigroup ${F_t}_{t\geq 0}$ on
$\mathbb{B}$ such that for some boundary point $\tau\in \partial\mathbb{B}$,
the admiss... | math.CV | we present a rigidity property of holomorphic generators on the open unit ball mathbbb of a hilbert space h namely if finhol mathbbbh is the generator of a oneparameter continuous semigroup f_t_tgeq 0 on mathbbb such that for some boundary point tauin partialmathbbb the admissible limit klimlimits_ztotaufracfxxtau30 th... | [['we', 'present', 'a', 'rigidity', 'property', 'of', 'holomorphic', 'generators', 'on', 'the', 'open', 'unit', 'ball', 'mathbbb', 'of', 'a', 'hilbert', 'space', 'h', 'namely', 'if', 'finhol', 'mathbbbh', 'is', 'the', 'generator', 'of', 'a', 'oneparameter', 'continuous', 'semigroup', 'f_t_tgeq', '0', 'on', 'mathbbb', '... | [-0.2152767396170874, 0.15778884358171905, -0.02999338539963474, -0.007329251215679153, -0.08904106772447727, -0.14538996025197665, 0.031243974576960792, 0.37542194508168164, -0.34340404232545774, -0.0064105157531341725, 0.16795532967020965, -0.30485604214957174, -0.09257151040590691, 0.18865171956772708, -0.1155933423... |
708.29 | The geometry of Minkowski spaces -- a survey. Part I | We survey elementary results in Minkowski spaces (i.e. finite dimensional
Banach spaces) that deserve to be collected together, and give simple proofs
for some of them. We place special emphasis on planar results. Many of these
results have often been rediscovered as lemmas to other results. In Part I we
cover the fo... | math.MG math.FA | we survey elementary results in minkowski spaces ie finite dimensional banach spaces that deserve to be collected together and give simple proofs for some of them we place special emphasis on planar results many of these results have often been rediscovered as lemmas to other results in part i we cover the following to... | [['we', 'survey', 'elementary', 'results', 'in', 'minkowski', 'spaces', 'ie', 'finite', 'dimensional', 'banach', 'spaces', 'that', 'deserve', 'to', 'be', 'collected', 'together', 'and', 'give', 'simple', 'proofs', 'for', 'some', 'of', 'them', 'we', 'place', 'special', 'emphasis', 'on', 'planar', 'results', 'many', 'of'... | [-0.12336378413211727, 0.029435965991050927, -0.08757816706352013, 0.13977681403288367, -0.15442601539981887, -0.1574631178866803, 0.02822590569399067, 0.4089742324209398, -0.2587582762785179, -0.19808319348304235, 0.1875821305750917, -0.3543130697144829, -0.11396383825442322, 0.2295080634582903, -0.1911473726774518, 0... |
708.2901 | Magnetogenesis from Cosmic String Loops | Large-scale coherent magnetic fields are observed in galaxies and clusters,
but their ultimate origin remains a mystery. We reconsider the prospects for
primordial magnetogenesis by a cosmic string network. We show that the magnetic
flux produced by long strings has been overestimated in the past, and give
improved e... | astro-ph hep-ph hep-th | largescale coherent magnetic fields are observed in galaxies and clusters but their ultimate origin remains a mystery we reconsider the prospects for primordial magnetogenesis by a cosmic string network we show that the magnetic flux produced by long strings has been overestimated in the past and give improved estimate... | [['largescale', 'coherent', 'magnetic', 'fields', 'are', 'observed', 'in', 'galaxies', 'and', 'clusters', 'but', 'their', 'ultimate', 'origin', 'remains', 'a', 'mystery', 'we', 'reconsider', 'the', 'prospects', 'for', 'primordial', 'magnetogenesis', 'by', 'a', 'cosmic', 'string', 'network', 'we', 'show', 'that', 'the',... | [-0.15512911041458108, 0.18359988462550475, -0.04260798362922502, 0.15352679841127825, -0.08082833072106985, -0.05088070401219038, -0.016470880121837214, 0.37992647586980405, -0.21886860175486306, -0.34367539058005586, 0.04009186994481068, -0.21863558775743885, -0.11416881781950686, 0.24221827645687768, 0.0471505277315... |
708.2902 | Monte Carlo simulation results for critical Casimir forces | The confinement of critical fluctuations in soft media induces critical
Casimir forces acting on the confining surfaces. The temperature and geometry
dependences of such forces are characterized by universal scaling functions. A
novel approach is presented to determine them for films via Monte Carlo
simulations of la... | cond-mat.stat-mech | the confinement of critical fluctuations in soft media induces critical casimir forces acting on the confining surfaces the temperature and geometry dependences of such forces are characterized by universal scaling functions a novel approach is presented to determine them for films via monte carlo simulations of lattic... | [['the', 'confinement', 'of', 'critical', 'fluctuations', 'in', 'soft', 'media', 'induces', 'critical', 'casimir', 'forces', 'acting', 'on', 'the', 'confining', 'surfaces', 'the', 'temperature', 'and', 'geometry', 'dependences', 'of', 'such', 'forces', 'are', 'characterized', 'by', 'universal', 'scaling', 'functions', ... | [-0.0923512367722155, 0.2051974872276994, -0.09473426205196037, 0.038047179630005055, 0.0003918831829320301, -0.13668958441121504, 0.027725468656916, 0.3965449965643612, -0.2329111646712673, -0.27725669785021717, 0.03319609895168634, -0.3166765124134889, -0.13625227340327745, 0.24534769347784194, 0.04608872235985473, 0... |
708.2903 | Fixed point scenario in the Two Higgs Doublet Model inspired by
degenerate vacua | We consider the renormalisation group flow of Higgs and Yukawa couplings
within the simplest non--supersymmetric two Higgs doublet extension of the
Standard Model (SM). In this model the couplings are adjusted so that the
multiple point principle (MPP) assumption, which implies the existence of a
large set of degener... | hep-ph | we consider the renormalisation group flow of higgs and yukawa couplings within the simplest nonsupersymmetric two higgs doublet extension of the standard model sm in this model the couplings are adjusted so that the multiple point principle mpp assumption which implies the existence of a large set of degenerate vacua ... | [['we', 'consider', 'the', 'renormalisation', 'group', 'flow', 'of', 'higgs', 'and', 'yukawa', 'couplings', 'within', 'the', 'simplest', 'nonsupersymmetric', 'two', 'higgs', 'doublet', 'extension', 'of', 'the', 'standard', 'model', 'sm', 'in', 'this', 'model', 'the', 'couplings', 'are', 'adjusted', 'so', 'that', 'the',... | [-0.12048374291503262, 0.23981693936940773, -0.02962068939507988, 0.17153791938433546, -0.06906304066682137, -0.23582190241952622, 0.03276495691879015, 0.2672140115005038, -0.23232434658443948, -0.27297309336350545, 0.018642002476170955, -0.2623294641288291, -0.010263815603378279, 0.08279528927156016, 0.056193002861140... |
708.2904 | Possible evidence of a ground level enhancement of muons in association
with a SWIFT Trigger | Starting from April 2007, a search for solar daily variation of the muon
intensity ($E_\mu >0.2$ GeV) at sea level and using two directional muon
telescopes is in progress. In this survey, several ground level enhancements
(GLEs) on the muon counting rate background have been found. Here, we highlight
one of them, ob... | astro-ph | starting from april 2007 a search for solar daily variation of the muon intensity e_mu 02 gev at sea level and using two directional muon telescopes is in progress in this survey several ground level enhancements gles on the muon counting rate background have been found here we highlight one of them observed in the ver... | [['starting', 'from', 'april', '2007', 'a', 'search', 'for', 'solar', 'daily', 'variation', 'of', 'the', 'muon', 'intensity', 'e_mu', '02', 'gev', 'at', 'sea', 'level', 'and', 'using', 'two', 'directional', 'muon', 'telescopes', 'is', 'in', 'progress', 'in', 'this', 'survey', 'several', 'ground', 'level', 'enhancements... | [-0.0926063289723354, 0.17112893987252362, -0.04108146103696969, 0.1337463452526536, -0.08927920095805751, -0.0930351366685281, 0.06189126810924114, 0.4204471427641931, -0.17872230432255834, -0.3988790341291597, 0.08537516365771798, -0.32292963819873466, -0.08727024449798905, 0.23445757598739594, -0.05742583465838774, ... |
708.2905 | Enhanced Higgs boson production and avoidance of CP-violation and FCNC
in the MPP inspired 2HDM | The multiple point principle (MPP) can be used to suppress non--diagonal
flavour transitions and CP violation in the two Higgs doublet extension of the
standard model. We discuss the quasi--fixed point scenario in the MPP inspired
two Higgs doublet model which leads to the enhanced production of Higgs
particles at th... | hep-ph | the multiple point principle mpp can be used to suppress nondiagonal flavour transitions and cp violation in the two higgs doublet extension of the standard model we discuss the quasifixed point scenario in the mpp inspired two higgs doublet model which leads to the enhanced production of higgs particles at the lhc if ... | [['the', 'multiple', 'point', 'principle', 'mpp', 'can', 'be', 'used', 'to', 'suppress', 'nondiagonal', 'flavour', 'transitions', 'and', 'cp', 'violation', 'in', 'the', 'two', 'higgs', 'doublet', 'extension', 'of', 'the', 'standard', 'model', 'we', 'discuss', 'the', 'quasifixed', 'point', 'scenario', 'in', 'the', 'mpp'... | [-0.10363942002155015, 0.2335357953922759, -0.030218549546432393, 0.17677738936015822, -0.0821333011684554, -0.26650952031145453, 0.040705560395445935, 0.2680457649945185, -0.2831978166138689, -0.29698761876929425, 0.03216850212052593, -0.2540294587660324, -0.029769507887098808, 0.05222286340973244, 0.03056232011796714... |
708.2906 | The general relativistic infinite plane | Uniform fields are one of the simplest and most pedagogically useful examples
in introductory courses on electrostatics or Newtonian gravity. In general
relativity there have been several proposals as to what constitutes a uniform
field. In this article we examine two metrics that can be considered the
general relati... | physics.ed-ph gr-qc hep-th | uniform fields are one of the simplest and most pedagogically useful examples in introductory courses on electrostatics or newtonian gravity in general relativity there have been several proposals as to what constitutes a uniform field in this article we examine two metrics that can be considered the general relativist... | [['uniform', 'fields', 'are', 'one', 'of', 'the', 'simplest', 'and', 'most', 'pedagogically', 'useful', 'examples', 'in', 'introductory', 'courses', 'on', 'electrostatics', 'or', 'newtonian', 'gravity', 'in', 'general', 'relativity', 'there', 'have', 'been', 'several', 'proposals', 'as', 'to', 'what', 'constitutes', 'a... | [-0.0865136314536524, 0.09577888713663009, -0.08599018592697878, 0.11486060728449861, -0.1381733932472831, -0.13288701568224948, -0.03495017583086307, 0.3458480561346887, -0.21986137388131027, -0.3122757875080543, 0.08804980046998441, -0.2843882170463212, -0.13672765791781394, 0.1898423902602148, -0.08940786517109552, ... |
708.2907 | Smallness of the cosmological constant and the multiple point principle | In this talk we argue that the breakdown of global symmetries in no--scale
supergravity (SUGRA), which ensures the vanishing of the vacuum energy density
near the physical vacuum, leads to a natural realisation of the multiple point
principle (MPP). In the MPP inspired SUGRA models the cosmological constant is
natura... | hep-ph | in this talk we argue that the breakdown of global symmetries in noscale supergravity sugra which ensures the vanishing of the vacuum energy density near the physical vacuum leads to a natural realisation of the multiple point principle mpp in the mpp inspired sugra models the cosmological constant is naturally tiny | [['in', 'this', 'talk', 'we', 'argue', 'that', 'the', 'breakdown', 'of', 'global', 'symmetries', 'in', 'noscale', 'supergravity', 'sugra', 'which', 'ensures', 'the', 'vanishing', 'of', 'the', 'vacuum', 'energy', 'density', 'near', 'the', 'physical', 'vacuum', 'leads', 'to', 'a', 'natural', 'realisation', 'of', 'the', '... | [-0.1613340381094638, 0.16629658626648142, -0.05704084388436932, 0.1010802790486053, -0.08118491667304553, -0.12201914372945241, 0.0059657803869021, 0.22959337067132926, -0.23864951026717238, -0.31016602286813305, 0.06814753245242744, -0.17912919523523135, -0.14297887847265778, 0.05268824955119806, -0.12399059088498939... |
708.2908 | Optimal control of molecular electronics by femtosecond laser pulses | Combining the features of molecular wires and femtosecond laser pulses gives
the unique opportunity to optically switch electron currents in molecular
devices with very high speed. Based on a weak-coupling approximation between
wire and leads a quantum master equation for the population dynamics and the
electric curr... | cond-mat.mes-hall | combining the features of molecular wires and femtosecond laser pulses gives the unique opportunity to optically switch electron currents in molecular devices with very high speed based on a weakcoupling approximation between wire and leads a quantum master equation for the population dynamics and the electric current ... | [['combining', 'the', 'features', 'of', 'molecular', 'wires', 'and', 'femtosecond', 'laser', 'pulses', 'gives', 'the', 'unique', 'opportunity', 'to', 'optically', 'switch', 'electron', 'currents', 'in', 'molecular', 'devices', 'with', 'very', 'high', 'speed', 'based', 'on', 'a', 'weakcoupling', 'approximation', 'betwee... | [-0.14601158601537095, 0.14513705068714466, -0.11066716677751862, -0.017024675424273338, -0.008299288058168246, -0.17239355881690605, 0.08716330076998272, 0.4445526424732779, -0.25550243429088293, -0.30362503772147564, 0.011293213294541166, -0.2418081544775236, -0.0713308557218426, 0.21463212954710012, 0.03004562333539... |
708.2909 | Testing the Topology of Reionization | The central overlap phase of cosmological hydrogen reionization is
fundamentally a change in the topology of ionized regions. Before overlap,
ionized bubbles grew in isolation. During overlap, they merge into a
percolating ionized medium, which fills an ever-increasing volume and
eventually replaces neutral gas throu... | astro-ph | the central overlap phase of cosmological hydrogen reionization is fundamentally a change in the topology of ionized regions before overlap ionized bubbles grew in isolation during overlap they merge into a percolating ionized medium which fills an everincreasing volume and eventually replaces neutral gas throughout th... | [['the', 'central', 'overlap', 'phase', 'of', 'cosmological', 'hydrogen', 'reionization', 'is', 'fundamentally', 'a', 'change', 'in', 'the', 'topology', 'of', 'ionized', 'regions', 'before', 'overlap', 'ionized', 'bubbles', 'grew', 'in', 'isolation', 'during', 'overlap', 'they', 'merge', 'into', 'a', 'percolating', 'io... | [-0.0691073333541998, 0.18136072053379773, -0.04222867295259696, 0.1014645175191406, -0.07606803339386228, -0.09375893178417585, 0.03344395274545477, 0.4151709754193245, -0.19535153158324456, -0.30817453051595084, 0.0735401604175676, -0.3101373201799254, -0.03609967570843955, 0.14947393369795972, 0.005589584281213235, ... |
708.291 | A Note on Agegraphic Dark Energy | Recently a new model of dynamical dark energy, or time-varying $\Lambda$, was
proposed by Cai [arXiv:0707.4049] by relating the energy density of quantum
fluctuations in a Minkowski space-time, namely $\rho_q \equiv 3 n^2 m_P^2/t^2$,
where $n\sim {\cal O}(1)$ and t is the cosmic time, to the present day dark
energy d... | hep-th astro-ph gr-qc hep-ph | recently a new model of dynamical dark energy or timevarying lambda was proposed by cai arxiv07074049 by relating the energy density of quantum fluctuations in a minkowski spacetime namely rho_q equiv 3 n2 m_p2t2 where nsim cal o1 and t is the cosmic time to the present day dark energy density in this note we show that... | [['recently', 'a', 'new', 'model', 'of', 'dynamical', 'dark', 'energy', 'or', 'timevarying', 'lambda', 'was', 'proposed', 'by', 'cai', 'arxiv07074049', 'by', 'relating', 'the', 'energy', 'density', 'of', 'quantum', 'fluctuations', 'in', 'a', 'minkowski', 'spacetime', 'namely', 'rho_q', 'equiv', '3', 'n2', 'm_p2t2', 'wh... | [-0.15020655951989087, 0.1888838429077768, -0.08853266388402829, 0.09004144005169237, -0.05927453088745079, -0.15145900239549343, 0.011286701162060013, 0.27892515226379755, -0.23666554562981434, -0.3824083785288, 0.042105055018778044, -0.2593681040368434, -0.04688772266496711, 0.11044377288983567, 0.011800323150701064,... |
708.2911 | Optimal Sequential Frame Synchronization | We consider the `one-shot frame synchronization problem' where a decoder
wants to locate a sync pattern at the output of a channel on the basis of
sequential observations. We assume that the sync pattern of length N starts
being emitted at a random time within some interval of size A, that
characterizes the asynchron... | cs.IT math.IT | we consider the oneshot frame synchronization problem where a decoder wants to locate a sync pattern at the output of a channel on the basis of sequential observations we assume that the sync pattern of length n starts being emitted at a random time within some interval of size a that characterizes the asynchronism lev... | [['we', 'consider', 'the', 'oneshot', 'frame', 'synchronization', 'problem', 'where', 'a', 'decoder', 'wants', 'to', 'locate', 'a', 'sync', 'pattern', 'at', 'the', 'output', 'of', 'a', 'channel', 'on', 'the', 'basis', 'of', 'sequential', 'observations', 'we', 'assume', 'that', 'the', 'sync', 'pattern', 'of', 'length', ... | [-0.17889384993087254, 0.13034339987758256, -0.05025398942877108, 0.05253870019066942, -0.051273735497751965, -0.2371971793212753, 0.13986015539654167, 0.37456549545229995, -0.2942681701730956, -0.2730912077406109, 0.10335521099895126, -0.28358207249938305, -0.12008002888810759, 0.1206532680242781, -0.05514502699598008... |
708.2912 | Isolating Triggered Star Formation | Galaxy pairs provide a potentially powerful means of studying triggered star
formation from galaxy interactions. We use a large cosmological N-body
simulation coupled with a well-tested semi-analytic substructure model to
demonstrate that the majority of galaxies in close pairs reside within cluster
or group-size hal... | astro-ph | galaxy pairs provide a potentially powerful means of studying triggered star formation from galaxy interactions we use a large cosmological nbody simulation coupled with a welltested semianalytic substructure model to demonstrate that the majority of galaxies in close pairs reside within cluster or groupsize halos and ... | [['galaxy', 'pairs', 'provide', 'a', 'potentially', 'powerful', 'means', 'of', 'studying', 'triggered', 'star', 'formation', 'from', 'galaxy', 'interactions', 'we', 'use', 'a', 'large', 'cosmological', 'nbody', 'simulation', 'coupled', 'with', 'a', 'welltested', 'semianalytic', 'substructure', 'model', 'to', 'demonstra... | [-0.08736799005350267, 0.06957872378031217, -0.06951326609696408, 0.13638188283914318, -0.0998505752297177, -0.031084210021553312, 0.049981416335767574, 0.41698119071803574, -0.11009309174734494, -0.38785676005242326, 0.021527841012085252, -0.27803301810301606, -0.03634257534955166, 0.1783065722070957, 0.01853160810584... |
708.2913 | Mapping Mass in the Local Universe | We only see a small fraction of the matter in the universe, but the rest
gives itself away by the impact of its gravity. Peculiar velocities have the
potential to be a powerful tool to trace this matter however previous peculiar
velocity surveys have struggled to meet their potential because of the large
errors on in... | astro-ph | we only see a small fraction of the matter in the universe but the rest gives itself away by the impact of its gravity peculiar velocities have the potential to be a powerful tool to trace this matter however previous peculiar velocity surveys have struggled to meet their potential because of the large errors on indivi... | [['we', 'only', 'see', 'a', 'small', 'fraction', 'of', 'the', 'matter', 'in', 'the', 'universe', 'but', 'the', 'rest', 'gives', 'itself', 'away', 'by', 'the', 'impact', 'of', 'its', 'gravity', 'peculiar', 'velocities', 'have', 'the', 'potential', 'to', 'be', 'a', 'powerful', 'tool', 'to', 'trace', 'this', 'matter', 'ho... | [-0.07198004181368797, 0.029870912781364826, -0.10967803371063835, 0.0844898662017879, -0.1997725033086517, -0.04173981707534307, 0.0829484603539886, 0.4279219163184482, -0.16264903461075084, -0.33797692937635204, 0.09913563739408528, -0.3199560448584716, -0.03815691252525949, 0.2210857927293287, -0.04288876205100678, ... |
708.2914 | The Coolest Stars in the Clouds: Unusual Red Supergiants in the
Magellanic Clouds | Red supergiants (RSGs) are a He-burning phase in the evolution of moderately
high mass stars (10-25 solar masses). The evolution of these stars,
particularly at low metallicities, is still poorly understood. The latest-type
RSGs in the Magellanic Clouds are cooler than the current evolutionary tracks
allow, occupying... | astro-ph | red supergiants rsgs are a heburning phase in the evolution of moderately high mass stars 1025 solar masses the evolution of these stars particularly at low metallicities is still poorly understood the latesttype rsgs in the magellanic clouds are cooler than the current evolutionary tracks allow occupying the region to... | [['red', 'supergiants', 'rsgs', 'are', 'a', 'heburning', 'phase', 'in', 'the', 'evolution', 'of', 'moderately', 'high', 'mass', 'stars', '1025', 'solar', 'masses', 'the', 'evolution', 'of', 'these', 'stars', 'particularly', 'at', 'low', 'metallicities', 'is', 'still', 'poorly', 'understood', 'the', 'latesttype', 'rsgs'... | [-0.07265984622490328, 0.21079306057919994, -0.08125718447610462, 0.09972526788403956, -0.06585495431006057, -0.07178329835526236, 0.05511060563544102, 0.4537837702328117, -0.1621484092541932, -0.35013313967426984, 0.07945129940170931, -0.29601684874222706, -0.03981308049069495, 0.17285339096508673, -0.0965328040963851... |
708.2915 | Molecular Recognition Effects in the Surface Diffusion of Large Organic
Molecules: The Case of Violet Lander | Violet Lander (VL) (C108H104) is a large organic molecule that when deposited
on Cu (110) exhibited lock-and-key like behavior (Otero et al., Nature Mater.
3, 779 (2004)). In this work we report on a detailed fully atomistic molecular
dynamics study of this phenomenon. Our results show that it has its physical
basis ... | cond-mat.mtrl-sci | violet lander vl c108h104 is a large organic molecule that when deposited on cu 110 exhibited lockandkey like behavior otero et al nature mater 3 779 2004 in this work we report on a detailed fully atomistic molecular dynamics study of this phenomenon our results show that it has its physical basis in the interplay of ... | [['violet', 'lander', 'vl', 'c108h104', 'is', 'a', 'large', 'organic', 'molecule', 'that', 'when', 'deposited', 'on', 'cu', '110', 'exhibited', 'lockandkey', 'like', 'behavior', 'otero', 'et', 'al', 'nature', 'mater', '3', '779', '2004', 'in', 'this', 'work', 'we', 'report', 'on', 'a', 'detailed', 'fully', 'atomistic',... | [-0.11196854574066636, 0.12025428752699793, -0.07828083798951029, 0.005548625688166602, -0.04859813611072145, -0.1069244262223181, 0.08926373677524296, 0.3906450665702945, -0.22433818408631181, -0.36010826841781013, 0.0012812514654605795, -0.2446187022877367, -0.22324992138892413, 0.1604901081931434, -0.014829379575032... |
708.2916 | The Evolution of the Chemical elements of the Universe | Spectroscopic observations of distant cosmological sources continue to
exhibit a surprising result; that the chemical abundance of the universe seems
to be approximately solar for the observed sources at redshifts of 5, 6, and
even 7, even though very few galaxies should have existed at these epochs and
the principal... | astro-ph | spectroscopic observations of distant cosmological sources continue to exhibit a surprising result that the chemical abundance of the universe seems to be approximately solar for the observed sources at redshifts of 5 6 and even 7 even though very few galaxies should have existed at these epochs and the principal star ... | [['spectroscopic', 'observations', 'of', 'distant', 'cosmological', 'sources', 'continue', 'to', 'exhibit', 'a', 'surprising', 'result', 'that', 'the', 'chemical', 'abundance', 'of', 'the', 'universe', 'seems', 'to', 'be', 'approximately', 'solar', 'for', 'the', 'observed', 'sources', 'at', 'redshifts', 'of', '5', '6',... | [-0.0717869780448599, 0.15933414996226333, -0.08067913071961323, 0.10765400070196657, -0.029357312283645482, -0.11611874769233278, 0.007467695706482254, 0.4171246959647136, -0.15327256136754555, -0.3916376663177316, 0.10351761641787059, -0.3262241734886792, 0.021733453066380165, 0.1761069495592322, 0.032018883723710014... |
708.2917 | Rounding by disorder of first-order quantum phase transitions: emergence
of quantum critical points | We give a heuristic argument for disorder rounding of a first order quantum
phase transition into a continuous phase transition. From both weak and strong
disorder analysis of the the N-color quantum Ashkin-Teller model in one spatial
dimension, we find that for $N \geq 3$, the first order transition is rounded
to a ... | cond-mat.dis-nn cond-mat.stat-mech | we give a heuristic argument for disorder rounding of a first order quantum phase transition into a continuous phase transition from both weak and strong disorder analysis of the the ncolor quantum ashkinteller model in one spatial dimension we find that for n geq 3 the first order transition is rounded to a continuous... | [['we', 'give', 'a', 'heuristic', 'argument', 'for', 'disorder', 'rounding', 'of', 'a', 'first', 'order', 'quantum', 'phase', 'transition', 'into', 'a', 'continuous', 'phase', 'transition', 'from', 'both', 'weak', 'and', 'strong', 'disorder', 'analysis', 'of', 'the', 'the', 'ncolor', 'quantum', 'ashkinteller', 'model',... | [-0.13129162664811772, 0.19963813112162127, -0.09530433949727851, 0.05821556773802373, -0.02431966418785473, -0.17748752509494528, 0.061212431151384056, 0.3434590765884003, -0.2383748077106877, -0.2395860352105676, 0.09199256343261088, -0.29238376929872456, -0.15597928070257275, 0.11367346382198426, 0.05805609191660411... |
708.2918 | The spin axes orbital alignment of both stars within the eclipsing
binary system V1143Cyg using the Rossiter-McLaughlin effect | Context: The Rossiter-McLaughlin (RM) effect, a rotational effect in
eclipsing systems, provides unique insight into the relative orientation of
stellar spin axes and orbital axes of eclipsing binary systems.
Aims: Our aim is to develop a robust method to analyze the RM effect in an
eclipsing system with two nearly... | astro-ph | context the rossitermclaughlin rm effect a rotational effect in eclipsing systems provides unique insight into the relative orientation of stellar spin axes and orbital axes of eclipsing binary systems aims our aim is to develop a robust method to analyze the rm effect in an eclipsing system with two nearly equally bri... | [['context', 'the', 'rossitermclaughlin', 'rm', 'effect', 'a', 'rotational', 'effect', 'in', 'eclipsing', 'systems', 'provides', 'unique', 'insight', 'into', 'the', 'relative', 'orientation', 'of', 'stellar', 'spin', 'axes', 'and', 'orbital', 'axes', 'of', 'eclipsing', 'binary', 'systems', 'aims', 'our', 'aim', 'is', '... | [-0.16698652090659985, 0.12169301639605373, -0.09572955940261875, 0.0214504872856196, -0.09337411899724159, -0.07900048970457232, 0.013024916876977505, 0.40618354168704207, -0.23203896784852668, -0.35388329310604094, 0.07471964115674175, -0.2744737469076522, -0.0785245783560656, 0.21436546873219572, -0.0493034557429174... |
708.2919 | Reaction-limited Colloidal Aggregation Induced by Salt and Inert
Polymers | Salt-induced aggregation of 20 nm colloidal silica is followed by light
transmission, which shows an a kinetic form exp[-(t/t_0)^{\alpha}], where
\alpha = 2.6 and t_0 is an empirical time constant which reflects the colloidal
stability. We found a power law dependence of t_0 on ionic strength, which can
be explained ... | cond-mat.soft cond-mat.mtrl-sci | saltinduced aggregation of 20 nm colloidal silica is followed by light transmission which shows an a kinetic form exptt_0alpha where alpha 26 and t_0 is an empirical time constant which reflects the colloidal stability we found a power law dependence of t_0 on ionic strength which can be explained by the classical dlvo... | [['saltinduced', 'aggregation', 'of', '20', 'nm', 'colloidal', 'silica', 'is', 'followed', 'by', 'light', 'transmission', 'which', 'shows', 'an', 'a', 'kinetic', 'form', 'exptt_0alpha', 'where', 'alpha', '26', 'and', 't_0', 'is', 'an', 'empirical', 'time', 'constant', 'which', 'reflects', 'the', 'colloidal', 'stability... | [-0.10201566096817506, 0.19402859878743076, -0.10686911282305195, 0.004567963535842186, -0.004822828349168018, -0.20243878548144031, 0.03402936297875308, 0.3675669712503835, -0.28429487245788765, -0.28439483428531787, 0.024168965611922538, -0.26916057834307017, -0.11699370981462426, 0.12846294084911125, 0.0208546959132... |
708.292 | Single polaron properties of the breathing-mode Hamiltonian | We investigate numerically various properties of the one-dimensional (1D)
breathing-mode polaron. We use an extension of a variational scheme to compute
the energies and wave-functions of the two lowest-energy eigenstates for any
momentum, as well as a scheme to compute directly the polaron Greens function.
We contra... | cond-mat.mtrl-sci | we investigate numerically various properties of the onedimensional 1d breathingmode polaron we use an extension of a variational scheme to compute the energies and wavefunctions of the two lowestenergy eigenstates for any momentum as well as a scheme to compute directly the polaron greens function we contrast these re... | [['we', 'investigate', 'numerically', 'various', 'properties', 'of', 'the', 'onedimensional', '1d', 'breathingmode', 'polaron', 'we', 'use', 'an', 'extension', 'of', 'a', 'variational', 'scheme', 'to', 'compute', 'the', 'energies', 'and', 'wavefunctions', 'of', 'the', 'two', 'lowestenergy', 'eigenstates', 'for', 'any',... | [-0.09812081580864149, 0.11692226765090537, -0.07966733664727292, 0.11847280900765983, -0.03686320558525957, -0.1182476277630944, 0.0675406797038106, 0.37051558320049766, -0.22221108138779397, -0.24346096273343842, 0.00039159736768048896, -0.26967935762494, -0.13073198992322693, 0.17516403697087085, 0.06808787462855312... |
708.2921 | On the DDVV Conjecture and the Comass in Calibrated Geometry (II) | In this paper, we proved P(n,3), which is an important part of the DDVV
conjecture. The general case will be treated in the next version of the paper.
| math.DG | in this paper we proved pn3 which is an important part of the ddvv conjecture the general case will be treated in the next version of the paper | [['in', 'this', 'paper', 'we', 'proved', 'pn3', 'which', 'is', 'an', 'important', 'part', 'of', 'the', 'ddvv', 'conjecture', 'the', 'general', 'case', 'will', 'be', 'treated', 'in', 'the', 'next', 'version', 'of', 'the', 'paper']] | [-0.13173541726012314, 0.054104646489577135, -0.07868694314467055, 0.06209192358489547, -0.007526246697774955, -0.0654068776805486, -0.06976350948181269, 0.2734805854436542, -0.2744949605715062, -0.2154563521700246, 0.1508422099369844, -0.20715021540776693, -0.22545680483537062, 0.18562524539551564, -0.1701410760038665... |
708.2922 | Recombination fluorescence in ultracold neutral plasmas | We present the first measurements and simulations of recombination
fluorescence in ultracold neutral plasmas. In contrast with previous work,
experiment and simulation are in significant disagreement. Comparison with a
recombination model suggests that the disagreement could be due to the high
energy portion of the e... | physics.atom-ph physics.plasm-ph | we present the first measurements and simulations of recombination fluorescence in ultracold neutral plasmas in contrast with previous work experiment and simulation are in significant disagreement comparison with a recombination model suggests that the disagreement could be due to the high energy portion of the electr... | [['we', 'present', 'the', 'first', 'measurements', 'and', 'simulations', 'of', 'recombination', 'fluorescence', 'in', 'ultracold', 'neutral', 'plasmas', 'in', 'contrast', 'with', 'previous', 'work', 'experiment', 'and', 'simulation', 'are', 'in', 'significant', 'disagreement', 'comparison', 'with', 'a', 'recombination'... | [-0.05040135090180402, 0.19991802847708423, -0.0284682409837842, 0.0685973083482513, 0.0395978442098521, -0.1243926672547867, 0.04567477182496952, 0.38450043313676796, -0.18798396004882606, -0.35468890121843244, -0.021415145046525648, -0.32342518283690835, -0.019684023811788406, 0.18246138637555362, 0.02879926198032460... |
708.2923 | Continuous opinion dynamics of multidimensional allocation problems
under bounded confidence: More dimensions lead to better chances for
consensus | We study multidimensional continuous opinion dynamics, where opinions are
nonnegative vectors which components sum up to one. Examples of such opinions
are budgets or other allocation vectors which display a distribution of a fixed
amount of ressource to n projects.
We use the opinion dynamics models of Deffuant-We... | physics.soc-ph | we study multidimensional continuous opinion dynamics where opinions are nonnegative vectors which components sum up to one examples of such opinions are budgets or other allocation vectors which display a distribution of a fixed amount of ressource to n projects we use the opinion dynamics models of deffuantweisbuch a... | [['we', 'study', 'multidimensional', 'continuous', 'opinion', 'dynamics', 'where', 'opinions', 'are', 'nonnegative', 'vectors', 'which', 'components', 'sum', 'up', 'to', 'one', 'examples', 'of', 'such', 'opinions', 'are', 'budgets', 'or', 'other', 'allocation', 'vectors', 'which', 'display', 'a', 'distribution', 'of', ... | [-0.12148806478203454, 0.131279349937364, -0.03885920245709441, 0.08414250746461915, -0.05997538553140132, -0.14825282231195952, 0.1218261383387104, 0.38496218086509554, -0.19712787141816646, -0.32970174692386056, 0.08863106141190814, -0.304373343937932, -0.09578460259854747, 0.14212527057960028, -0.037846027457777855,... |
708.2924 | Cuprate Fermi orbits and Fermi arcs: the effect of short-range
antiferromagnetic order | We consider the effect of a short antiferromagnetic correlation length $\xi$
on the electronic bandstructure of the underdoped cuprates. Starting with a
Fermi-surface topology similar to that detected in magnetic quantum-oscillation
experiments, we show that a reduced $\xi$ gives an assymmetric broadening of
the quas... | cond-mat.supr-con cond-mat.str-el | we consider the effect of a short antiferromagnetic correlation length xi on the electronic bandstructure of the underdoped cuprates starting with a fermisurface topology similar to that detected in magnetic quantumoscillation experiments we show that a reduced xi gives an assymmetric broadening of the quasiparticle di... | [['we', 'consider', 'the', 'effect', 'of', 'a', 'short', 'antiferromagnetic', 'correlation', 'length', 'xi', 'on', 'the', 'electronic', 'bandstructure', 'of', 'the', 'underdoped', 'cuprates', 'starting', 'with', 'a', 'fermisurface', 'topology', 'similar', 'to', 'that', 'detected', 'in', 'magnetic', 'quantumoscillation'... | [-0.20397893525660038, 0.1838187990933875, -0.07345000089013151, 0.1251542227338567, -0.07714921048110616, -0.12364131933177955, 0.07574375205565177, 0.34633684094712536, -0.24736411395133473, -0.2970890506902443, -0.07263048563410328, -0.3622412714591649, -0.11082742725349297, 0.1953564509811778, -0.003285563309743468... |
708.2925 | Using Molecules to Measure Nuclear Spin-Dependent Parity Violation | Nuclear spin-dependent parity violation arises from weak interactions between
electrons and nucleons, and from nuclear anapole moments. We outline a method
to measure such effects, using a Stark-interference technique to determine the
mixing between opposite-parity rotational/hyperfine levels of ground-state
molecule... | physics.atom-ph nucl-ex | nuclear spindependent parity violation arises from weak interactions between electrons and nucleons and from nuclear anapole moments we outline a method to measure such effects using a starkinterference technique to determine the mixing between oppositeparity rotationalhyperfine levels of groundstate molecules the tech... | [['nuclear', 'spindependent', 'parity', 'violation', 'arises', 'from', 'weak', 'interactions', 'between', 'electrons', 'and', 'nucleons', 'and', 'from', 'nuclear', 'anapole', 'moments', 'we', 'outline', 'a', 'method', 'to', 'measure', 'such', 'effects', 'using', 'a', 'starkinterference', 'technique', 'to', 'determine',... | [-0.07846574371003291, 0.20927363220457132, -0.03394712576137662, 0.1623347115207028, -0.03563531604293105, -0.11962935261355785, 0.09971696954801099, 0.37891391746990094, -0.24137679241936316, -0.32918133521331594, -0.07313685765786265, -0.28305391719347084, -0.015996209454613847, 0.1773785561347356, 0.102988481080135... |
708.2926 | Quantum and classical criticalities in the frustrated two-leg Heisenberg
ladder | This talk was about the frustration-induced criticality in the
antiferromagnetic Heisenberg model on the two-leg ladder with exchange
interactions along the chains, rungs, and diagonals, and also about the effect
of thermal fluctuations on this criticlity. The method used is the bond
mean-field theory, which is based... | cond-mat.str-el | this talk was about the frustrationinduced criticality in the antiferromagnetic heisenberg model on the twoleg ladder with exchange interactions along the chains rungs and diagonals and also about the effect of thermal fluctuations on this criticlity the method used is the bond meanfield theory which is based on the jo... | [['this', 'talk', 'was', 'about', 'the', 'frustrationinduced', 'criticality', 'in', 'the', 'antiferromagnetic', 'heisenberg', 'model', 'on', 'the', 'twoleg', 'ladder', 'with', 'exchange', 'interactions', 'along', 'the', 'chains', 'rungs', 'and', 'diagonals', 'and', 'also', 'about', 'the', 'effect', 'of', 'thermal', 'fl... | [-0.1429281577535243, 0.1970064444804048, -0.05545400613035266, 0.03848400875555733, -0.05471294653792697, -0.09202411424099322, 0.049663571767082595, 0.3545888254800475, -0.20942727761365562, -0.25617300880601607, 0.0905717661273273, -0.3594514512827238, -0.14782265608804862, 0.14581326628384372, 0.05070615972740104, ... |
708.2927 | The VSL Discussion: What Does Variable Speed of Light Mean and Should we
be Allowed to Think About ? | In the past years, variable speed of light (VSL) theories have been of
growing interest but also a subject of controversial discussion. They have been
accused both for tautologies and for violating special relativity, and concerns
have been expressed about the validity of such approaches in general (e.g.
Ellis, astro... | physics.gen-ph | in the past years variable speed of light vsl theories have been of growing interest but also a subject of controversial discussion they have been accused both for tautologies and for violating special relativity and concerns have been expressed about the validity of such approaches in general eg ellis astroph0703751 w... | [['in', 'the', 'past', 'years', 'variable', 'speed', 'of', 'light', 'vsl', 'theories', 'have', 'been', 'of', 'growing', 'interest', 'but', 'also', 'a', 'subject', 'of', 'controversial', 'discussion', 'they', 'have', 'been', 'accused', 'both', 'for', 'tautologies', 'and', 'for', 'violating', 'special', 'relativity', 'an... | [-0.07894619021340962, 0.0741128669084086, -0.09801248737985825, 0.10591374660612314, -0.1558030829704427, -0.1657388836278447, 0.04737007824020678, 0.33873476808574715, -0.13576820927563232, -0.33643291814422066, 0.15851067878342198, -0.29345093760941804, -0.11399202403920859, 0.2015896459463863, -0.15501805062877475,... |
708.2928 | The reciprocity law for the twisted second moment of Dirichlet
L-functions | We produce a new proof of the reciprocity law for the twisted second moment
of Dirichlet L-functions that was recently proved by Conrey. Our method is to
analyze certain two-variable sums where the variables satisfy a linear
congruence. We show that these sums satisfy an elegant reciprocity formula. In
the case that ... | math.NT | we produce a new proof of the reciprocity law for the twisted second moment of dirichlet lfunctions that was recently proved by conrey our method is to analyze certain twovariable sums where the variables satisfy a linear congruence we show that these sums satisfy an elegant reciprocity formula in the case that the mod... | [['we', 'produce', 'a', 'new', 'proof', 'of', 'the', 'reciprocity', 'law', 'for', 'the', 'twisted', 'second', 'moment', 'of', 'dirichlet', 'lfunctions', 'that', 'was', 'recently', 'proved', 'by', 'conrey', 'our', 'method', 'is', 'to', 'analyze', 'certain', 'twovariable', 'sums', 'where', 'the', 'variables', 'satisfy', ... | [-0.1799436942192501, 0.06459070642190402, -0.14557922278358948, 0.1254119551606776, -0.15056706298592276, -0.11871487736145313, 0.028100478244763423, 0.278688317143369, -0.31351304919212714, -0.24106993940364485, 0.07163863358671252, -0.2185723134905271, -0.1931271444706396, 0.24668740117173085, -0.0953748104772691, 0... |
708.2929 | On the origin of radio core emission in radio-quiet quasars | We present a model for the radio emission from radio-quiet quasar nuclei. We
show that a thermal origin for the high brightness temperature, flat spectrum
point sources (known as radio ``cores'') is possible provided the emitting
region is hot and optically-thin. We hence demonstrate that optically-thin
bremsstrahlun... | astro-ph | we present a model for the radio emission from radioquiet quasar nuclei we show that a thermal origin for the high brightness temperature flat spectrum point sources known as radio cores is possible provided the emitting region is hot and opticallythin we hence demonstrate that opticallythin bremsstrahlung from a slow ... | [['we', 'present', 'a', 'model', 'for', 'the', 'radio', 'emission', 'from', 'radioquiet', 'quasar', 'nuclei', 'we', 'show', 'that', 'a', 'thermal', 'origin', 'for', 'the', 'high', 'brightness', 'temperature', 'flat', 'spectrum', 'point', 'sources', 'known', 'as', 'radio', 'cores', 'is', 'possible', 'provided', 'the', '... | [-0.052857728174587455, 0.1409330520750894, -0.051741935409852675, 0.15911996418033, -0.13912800281260038, -0.10014412197244676, 0.05059483815017664, 0.4967961344267661, -0.16173311185877398, -0.2881962419857886, 0.07440771375147193, -0.26649201415938223, -0.01896583639257433, 0.2311734077862742, 0.00800121928246855, -... |
708.293 | Fluctuations and symmetry in the speed and direction of the jets of
SS433 on different timescales | ABRIDGED We present new results on the variations in speed and direction of
the jet bolides in the Galactic microquasar SS433, from high resolution
spectra, taken with the ESO 3.6-m New Technology Telescope almost nightly over
0.4 of a precession cycle. We find: (i) These data exhibit multiple ejections
within most 2... | astro-ph | abridged we present new results on the variations in speed and direction of the jet bolides in the galactic microquasar ss433 from high resolution spectra taken with the eso 36m new technology telescope almost nightly over 04 of a precession cycle we find i these data exhibit multiple ejections within most 24hour perio... | [['abridged', 'we', 'present', 'new', 'results', 'on', 'the', 'variations', 'in', 'speed', 'and', 'direction', 'of', 'the', 'jet', 'bolides', 'in', 'the', 'galactic', 'microquasar', 'ss433', 'from', 'high', 'resolution', 'spectra', 'taken', 'with', 'the', 'eso', '36m', 'new', 'technology', 'telescope', 'almost', 'night... | [-0.13591585344038887, 0.14008538173265708, -0.08416356422483574, 0.05048275616944067, -0.07329781995292088, -0.08078420595554707, 0.03676806420788111, 0.4570135955893716, -0.231349015610122, -0.3214961337399973, 0.09608443952373107, -0.25452975956454615, -0.09091549562903974, 0.23311051992381843, -0.06857875524929818,... |
708.2931 | Structure-Activity Relationship Investigation of Some New Tetracyclines
by Electronic Index Methodology | Tetracyclines are an old class of molecules that constitute a broad-spectrum
antibiotics. Since the first member of tetracycline family were isolated, the
clinical importance of these compounds as therapeutic and prophylactic agents
against a wide range of infections has stimulated efforts to define their mode
of act... | q-bio.BM physics.bio-ph | tetracyclines are an old class of molecules that constitute a broadspectrum antibiotics since the first member of tetracycline family were isolated the clinical importance of these compounds as therapeutic and prophylactic agents against a wide range of infections has stimulated efforts to define their mode of action a... | [['tetracyclines', 'are', 'an', 'old', 'class', 'of', 'molecules', 'that', 'constitute', 'a', 'broadspectrum', 'antibiotics', 'since', 'the', 'first', 'member', 'of', 'tetracycline', 'family', 'were', 'isolated', 'the', 'clinical', 'importance', 'of', 'these', 'compounds', 'as', 'therapeutic', 'and', 'prophylactic', 'a... | [-0.03476578825373306, 0.05184271229851826, -0.07633821306646699, 0.05656099359960839, -0.03447482647768791, -0.12867455887155504, 0.07657469905421345, 0.3816154064843431, -0.20096281982033462, -0.307134918609841, 0.08796045239028495, -0.2932953369988051, -0.2066112169284477, 0.21988273080165122, -0.06298981593459353, ... |
708.2932 | Broken Pair Model: A viable Alterative to the Shell Model for
Odd-Spherical Nuclei | The broken pair model has been developed earlier as an useful approximation
to the nuclear shell model for even-even nuclei. It is extended and developed
here to include odd nuclei too. The model is then applied successfully in the
Zr region, using two different sets of matrix elements, the empirical and the
realisti... | nucl-th | the broken pair model has been developed earlier as an useful approximation to the nuclear shell model for eveneven nuclei it is extended and developed here to include odd nuclei too the model is then applied successfully in the zr region using two different sets of matrix elements the empirical and the realistic susse... | [['the', 'broken', 'pair', 'model', 'has', 'been', 'developed', 'earlier', 'as', 'an', 'useful', 'approximation', 'to', 'the', 'nuclear', 'shell', 'model', 'for', 'eveneven', 'nuclei', 'it', 'is', 'extended', 'and', 'developed', 'here', 'to', 'include', 'odd', 'nuclei', 'too', 'the', 'model', 'is', 'then', 'applied', '... | [0.007360618140193678, 0.08681370433121283, -0.08256670633064848, 0.12933592911022493, 0.0037999922975099514, -0.16759861612670302, 0.023516685657557986, 0.42479533174385625, -0.20008031573767462, -0.317841820213722, 0.058499879274417514, -0.30823963811798466, -0.08374655122558276, 0.14759250501048796, 0.05513556746431... |
708.2933 | SUSY Shape-Invariant Hamiltonians for the Generalized Dirac-Coulomb
Problem | A spin $\frac 12$ relativistic particle described by a general potential in
terms of the sum of the Coulomb potential with a Lorentz scalar potential is
investigated via supersymmetry in quantum mechanics.
| hep-th | a spin frac 12 relativistic particle described by a general potential in terms of the sum of the coulomb potential with a lorentz scalar potential is investigated via supersymmetry in quantum mechanics | [['a', 'spin', 'frac', '12', 'relativistic', 'particle', 'described', 'by', 'a', 'general', 'potential', 'in', 'terms', 'of', 'the', 'sum', 'of', 'the', 'coulomb', 'potential', 'with', 'a', 'lorentz', 'scalar', 'potential', 'is', 'investigated', 'via', 'supersymmetry', 'in', 'quantum', 'mechanics']] | [-0.13077341311145574, 0.2133299214183353, -0.02530953547102399, 0.08396315482605132, 0.01896283167297952, -0.18754789904050995, -0.035840313583321404, 0.263484051451087, -0.1938385713729076, -0.2573951670783572, -0.010097412603499833, -0.26819838050869294, -0.145320737734437, 0.1124969592965499, 0.0393281152646523, 0.... |
708.2934 | Observation of Galactic Sources of Very High Energy Gamma-Rays with the
MAGIC Telescope | The MAGIC telescope with its 17m diameter mirror is today the largest
operating single-dish Imaging Air Cherenkov Telescope (IACT). It is located on
the Canary Island La Palma, at an altitude of 2200m above sea level, as part of
the Roque de los Muchachos European Northern Observatory. The MAGIC telescope
detects cel... | astro-ph | the magic telescope with its 17m diameter mirror is today the largest operating singledish imaging air cherenkov telescope iact it is located on the canary island la palma at an altitude of 2200m above sea level as part of the roque de los muchachos european northern observatory the magic telescope detects celestial ve... | [['the', 'magic', 'telescope', 'with', 'its', '17m', 'diameter', 'mirror', 'is', 'today', 'the', 'largest', 'operating', 'singledish', 'imaging', 'air', 'cherenkov', 'telescope', 'iact', 'it', 'is', 'located', 'on', 'the', 'canary', 'island', 'la', 'palma', 'at', 'an', 'altitude', 'of', '2200m', 'above', 'sea', 'level'... | [-0.08423712709425334, 0.19914383634688604, -0.03512411372601923, 0.21751327344025997, -0.1238024951890111, -0.08643305601978327, 0.02356517481443993, 0.4176506915966333, -0.09693752854502112, -0.43183193562583905, 0.11159323120462093, -0.3630533405042932, -0.009446399973042436, 0.27634048573988473, -0.0236610302748947... |
708.2935 | Loss of entanglement in quantum mechanics due to the use of realistic
measuring rods | We show that the use of real measuring rods in quantum mechanics places a
fundamental gravitational limit to the level of entanglement that one can
ultimately achieve in quantum systems. The result can be seen as a direct
consequence of the fundamental gravitational limitations in the measurements of
length and time ... | quant-ph gr-qc | we show that the use of real measuring rods in quantum mechanics places a fundamental gravitational limit to the level of entanglement that one can ultimately achieve in quantum systems the result can be seen as a direct consequence of the fundamental gravitational limitations in the measurements of length and time in ... | [['we', 'show', 'that', 'the', 'use', 'of', 'real', 'measuring', 'rods', 'in', 'quantum', 'mechanics', 'places', 'a', 'fundamental', 'gravitational', 'limit', 'to', 'the', 'level', 'of', 'entanglement', 'that', 'one', 'can', 'ultimately', 'achieve', 'in', 'quantum', 'systems', 'the', 'result', 'can', 'be', 'seen', 'as'... | [-0.14405231356201037, 0.1571039744902035, -0.10965294348941722, 0.063531778883976, -0.00479463848587073, -0.11214893866653397, 0.03617056197172005, 0.3072534166276455, -0.29561830364482505, -0.29741263780480537, 0.07780295571568094, -0.2318580040813122, -0.15622579202738027, 0.27099557897784343, -0.05410381126493006, ... |
708.2936 | Priority Queue Based on Multilevel Prefix Tree | Tree structures are very often used data structures. Among ordered types of
trees there are many variants whose basic operations such as insert, delete,
search, delete-min are characterized by logarithmic time complexity. In the
article I am going to present the structure whose time complexity for each of
the above o... | cs.DS | tree structures are very often used data structures among ordered types of trees there are many variants whose basic operations such as insert delete search deletemin are characterized by logarithmic time complexity in the article i am going to present the structure whose time complexity for each of the above operation... | [['tree', 'structures', 'are', 'very', 'often', 'used', 'data', 'structures', 'among', 'ordered', 'types', 'of', 'trees', 'there', 'are', 'many', 'variants', 'whose', 'basic', 'operations', 'such', 'as', 'insert', 'delete', 'search', 'deletemin', 'are', 'characterized', 'by', 'logarithmic', 'time', 'complexity', 'in', ... | [-0.16507879370870068, 0.16064923936128617, -0.03288562893308699, 0.07130125797912479, -0.09873674386739731, -0.15994226399017497, 0.12973478444712236, 0.3698359310925007, -0.33930224750936033, -0.3403156419582665, 0.13870312050078065, -0.2714283971562982, -0.08693735612183809, 0.1178104520458728, -0.044874097514897585... |
708.2937 | On the Connection of Anisotropic Conductivity to Tip Induced Space
Charge Layers in Scanning Tunneling Spectroscopy of p-doped GaAs | The electronic properties of shallow acceptors in p-doped GaAs{110} are
investigated with scanning tunneling microscopy at low temperature. Shallow
acceptors are known to exhibit distinct triangular contrasts in STM images for
certain bias voltages. Spatially resolved I(V)-spectroscopy is performed to
identify their ... | cond-mat.mes-hall cond-mat.dis-nn | the electronic properties of shallow acceptors in pdoped gaas110 are investigated with scanning tunneling microscopy at low temperature shallow acceptors are known to exhibit distinct triangular contrasts in stm images for certain bias voltages spatially resolved ivspectroscopy is performed to identify their energetic ... | [['the', 'electronic', 'properties', 'of', 'shallow', 'acceptors', 'in', 'pdoped', 'gaas110', 'are', 'investigated', 'with', 'scanning', 'tunneling', 'microscopy', 'at', 'low', 'temperature', 'shallow', 'acceptors', 'are', 'known', 'to', 'exhibit', 'distinct', 'triangular', 'contrasts', 'in', 'stm', 'images', 'for', 'c... | [-0.14058707744504015, 0.12965521869191435, -0.041952908058495574, 0.07156200440908833, -0.01949365081770035, -0.20806431671371683, 0.059136623248438505, 0.4451169023290277, -0.27834163871593776, -0.320240395112584, -0.0064300898414027564, -0.32641437428537756, -0.10435245008363078, 0.2003580188267127, -0.0122993510083... |
708.2938 | Neck Pinching Dynamics Under Mean Curvature Flow | In this paper we study motion of surfaces of revolution under the mean
curvature flow. For an open set of initial conditions close to cylindrical
surfaces we show that the solution forms a "neck" which pinches in a finite
time at a single point. We also obtain a detailed description of the neck
pinching process.
| math.AP math.DG | in this paper we study motion of surfaces of revolution under the mean curvature flow for an open set of initial conditions close to cylindrical surfaces we show that the solution forms a neck which pinches in a finite time at a single point we also obtain a detailed description of the neck pinching process | [['in', 'this', 'paper', 'we', 'study', 'motion', 'of', 'surfaces', 'of', 'revolution', 'under', 'the', 'mean', 'curvature', 'flow', 'for', 'an', 'open', 'set', 'of', 'initial', 'conditions', 'close', 'to', 'cylindrical', 'surfaces', 'we', 'show', 'that', 'the', 'solution', 'forms', 'a', 'neck', 'which', 'pinches', 'in... | [-0.16396712929179721, 0.08160505068980538, -0.15818342147395015, 0.027865961578374315, -0.014613030626523223, -0.06713485060767695, 0.03233454158233309, 0.3705050263215195, -0.2736176602627066, -0.21738205535167998, 0.11409735618243841, -0.23649723455309868, -0.1406080732291395, 0.20481721459125932, -0.114131971922787... |
708.2939 | Observing the Dark Scalar Doublet and its Impact on the Standard-Model
Higgs Boson at Colliders | If the Standard Model of particle interactions is extended to include a
second scalar doublet $[H^{+},(H^{0}+iA^{0})/\sqrt{2}]$, which is odd under an
unbroken Z_{2} discrete symmetry, it may be called the $dark$ scalar doublet,
because its lightest neutral member, say H^{0}, is one posssible component for
the dark m... | hep-ph | if the standard model of particle interactions is extended to include a second scalar doublet hh0ia0sqrt2 which is odd under an unbroken z_2 discrete symmetry it may be called the dark scalar doublet because its lightest neutral member say h0 is one posssible component for the dark matter of the universe we discuss the... | [['if', 'the', 'standard', 'model', 'of', 'particle', 'interactions', 'is', 'extended', 'to', 'include', 'a', 'second', 'scalar', 'doublet', 'hh0ia0sqrt2', 'which', 'is', 'odd', 'under', 'an', 'unbroken', 'z_2', 'discrete', 'symmetry', 'it', 'may', 'be', 'called', 'the', 'dark', 'scalar', 'doublet', 'because', 'its', '... | [-0.12916518705795801, 0.24027709926509566, -0.07917772568876187, 0.1752008182001705, -0.13787577184848487, -0.24012054884603815, -0.06899312984086978, 0.2976984464305291, -0.2103415056405103, -0.2832795305936167, 0.01858973020242284, -0.24699395249152314, 0.007374204037225117, 0.030983976502244805, 0.07024803132567879... |
708.294 | Nonequilibrium steady state thermodynamics and fluctuations for
stochastic systems | We use the work done on and the heat removed from a system to maintain it in
a nonequilibrium steady state for a thermodynamic-like description of such a
system as well as of its fluctuations. Based on a generalized Onsager-Machlup
theory for nonequilibrium steady states we indicate two ambiguities, not
present in an... | cond-mat.stat-mech | we use the work done on and the heat removed from a system to maintain it in a nonequilibrium steady state for a thermodynamiclike description of such a system as well as of its fluctuations based on a generalized onsagermachlup theory for nonequilibrium steady states we indicate two ambiguities not present in an equil... | [['we', 'use', 'the', 'work', 'done', 'on', 'and', 'the', 'heat', 'removed', 'from', 'a', 'system', 'to', 'maintain', 'it', 'in', 'a', 'nonequilibrium', 'steady', 'state', 'for', 'a', 'thermodynamiclike', 'description', 'of', 'such', 'a', 'system', 'as', 'well', 'as', 'of', 'its', 'fluctuations', 'based', 'on', 'a', 'g... | [-0.11757791964144353, 0.12563524473101706, -0.10036703921060942, 0.06378723705220504, -0.02194753575232431, -0.1154928288957071, 0.07945631595518572, 0.29811180165291007, -0.29773199457135163, -0.2965485198566547, 0.0983257520073865, -0.2643816268027446, -0.11434967934495642, 0.2483792281992039, -0.04425869104948402, ... |
708.2941 | Hook modules for general linear groups | For an arbitrary infinite field k of characteristic p > 0, we describe the
structure of a block of the algebraic monoid M_n(k) (all n x n matrices over
k), or, equivalently, a block of the Schur algebra S(n,p), whose simple modules
are indexed by p-hook partitions. The result is known; we give an elementary
and self-... | math.RT math.GR | for an arbitrary infinite field k of characteristic p 0 we describe the structure of a block of the algebraic monoid m_nk all n x n matrices over k or equivalently a block of the schur algebra snp whose simple modules are indexed by phook partitions the result is known we give an elementary and selfcontained proof base... | [['for', 'an', 'arbitrary', 'infinite', 'field', 'k', 'of', 'characteristic', 'p', '0', 'we', 'describe', 'the', 'structure', 'of', 'a', 'block', 'of', 'the', 'algebraic', 'monoid', 'm_nk', 'all', 'n', 'x', 'n', 'matrices', 'over', 'k', 'or', 'equivalently', 'a', 'block', 'of', 'the', 'schur', 'algebra', 'snp', 'whose'... | [-0.17997551941381837, 0.11683667858408255, -0.0657978769029594, 0.030077027283065643, -0.08200014962952722, -0.18308234452356206, 0.031449723335552134, 0.2879327528730587, -0.304970016120933, -0.22717846401415212, 0.08701895691316437, -0.21583161427406594, -0.14842112279223296, 0.203971494461358, -0.04089311430989592,... |
708.2942 | A Comprehensive Analysis of Swift/XRT Data: III. Jet Break Candidates in
X-ray and Optical Afterglow Lightcurves | The Swift/XRT data of 179 GRBs (from 050124 to 070129) and the optical
afterglow data of 57 pre- and post-Swift GRBs are analyzed, in order to
systematically investigate the jet-like breaks in the X-ray and optical
afterglow lightcurves. We find that not a single burst can be included in the
``Platinum'' sample, in w... | astro-ph | the swiftxrt data of 179 grbs from 050124 to 070129 and the optical afterglow data of 57 pre and postswift grbs are analyzed in order to systematically investigate the jetlike breaks in the xray and optical afterglow lightcurves we find that not a single burst can be included in the platinum sample in which the data sa... | [['the', 'swiftxrt', 'data', 'of', '179', 'grbs', 'from', '050124', 'to', '070129', 'and', 'the', 'optical', 'afterglow', 'data', 'of', '57', 'pre', 'and', 'postswift', 'grbs', 'are', 'analyzed', 'in', 'order', 'to', 'systematically', 'investigate', 'the', 'jetlike', 'breaks', 'in', 'the', 'xray', 'and', 'optical', 'af... | [-0.06893637676851928, 0.14038927050823732, -0.0825681369002726, 0.1600097007797119, -0.09580765777736433, -0.1329921490213202, 0.07278556877851382, 0.4737288322767008, -0.1986450335569354, -0.37739014316193914, 0.06865733922735977, -0.34078273862287717, -0.0018103511463052925, 0.22546385307682326, 0.000843844969164241... |
708.2943 | Dark Energy or Apparent Acceleration Due to a Relativistic Cosmological
Model More Complex than FLRW? | We use the Szekeres inhomogeneous relativistic models in order to fit
supernova combined data sets. We show that with a choice of the spatial
curvature function that is guided by current observations, the models fit the
supernova data almost as well as the LCDM model without requiring a dark energy
component. The Sze... | astro-ph gr-qc hep-th | we use the szekeres inhomogeneous relativistic models in order to fit supernova combined data sets we show that with a choice of the spatial curvature function that is guided by current observations the models fit the supernova data almost as well as the lcdm model without requiring a dark energy component the szekeres... | [['we', 'use', 'the', 'szekeres', 'inhomogeneous', 'relativistic', 'models', 'in', 'order', 'to', 'fit', 'supernova', 'combined', 'data', 'sets', 'we', 'show', 'that', 'with', 'a', 'choice', 'of', 'the', 'spatial', 'curvature', 'function', 'that', 'is', 'guided', 'by', 'current', 'observations', 'the', 'models', 'fit',... | [-0.04838767947980782, 0.05987659299030161, -0.10212190096898303, 0.13323769728991797, -0.12385265057632973, -0.13052434717806485, -0.04122061543394583, 0.3937273614785888, -0.23409025839992337, -0.3412167983084031, 0.0951574458691806, -0.273785295222163, -0.0774700057764466, 0.17264629632700235, -0.0001780703904797564... |
708.2944 | The K-Theory of Toeplitz C*-Algebras of Right-Angled Artin Groups | To a graph $\Gamma$ one can associate a C^*-algebra $C^*(\Gamma)$ generated
by isometries. Such $C^*$-algebras were studied recently by Crisp and Laca.
They are a special case of the Toeplitz C^*-algebras $\mathcal{T}(G, P)$
associated to quasi-latice ordered groups (G, P) introduced by Nica. Crisp and
Laca proved th... | math.OA math.KT | to a graph gamma one can associate a calgebra cgamma generated by isometries such calgebras were studied recently by crisp and laca they are a special case of the toeplitz calgebras mathcaltg p associated to quasilatice ordered groups g p introduced by nica crisp and laca proved that the so called boundary quotients c_... | [['to', 'a', 'graph', 'gamma', 'one', 'can', 'associate', 'a', 'calgebra', 'cgamma', 'generated', 'by', 'isometries', 'such', 'calgebras', 'were', 'studied', 'recently', 'by', 'crisp', 'and', 'laca', 'they', 'are', 'a', 'special', 'case', 'of', 'the', 'toeplitz', 'calgebras', 'mathcaltg', 'p', 'associated', 'to', 'quas... | [-0.11428536093410324, 0.16979036259213257, -0.061450570295838745, 0.05983757646103828, -0.11332759089932284, -0.14303666062050444, 0.015904948732350023, 0.4116426159353817, -0.3274196100366466, -0.21816605117295265, 0.10809087323517923, -0.29159634275094826, -0.10551636741250096, 0.17533502393840428, -0.10058184249792... |
708.2945 | Tackling the Fermionic Sign Problem in the Auxiliary-Field Monte Carlo
Method | We explore a novel and straightforward solution to the sign problem that has
plagued the Auxiliary-field Monte Carlo (AFMC) method applied to many-body
systems for more than a decade. We present a solution to the sign problem that
has plagued the Auxiliary-field Monte Carlo (AFMC) method for more than a
decade and re... | nucl-th | we explore a novel and straightforward solution to the sign problem that has plagued the auxiliaryfield monte carlo afmc method applied to manybody systems for more than a decade we present a solution to the sign problem that has plagued the auxiliaryfield monte carlo afmc method for more than a decade and report a bre... | [['we', 'explore', 'a', 'novel', 'and', 'straightforward', 'solution', 'to', 'the', 'sign', 'problem', 'that', 'has', 'plagued', 'the', 'auxiliaryfield', 'monte', 'carlo', 'afmc', 'method', 'applied', 'to', 'manybody', 'systems', 'for', 'more', 'than', 'a', 'decade', 'we', 'present', 'a', 'solution', 'to', 'the', 'sign... | [-0.08481484702055793, 0.011692340171822671, -0.11257517587895809, 0.09650888488617505, -0.04097975720913055, -0.1584555338806567, 0.048938292188548976, 0.4175339640024003, -0.20969745746991608, -0.33587567845171085, 0.07905003460898494, -0.3027034819752679, -0.1405445919110534, 0.259494521924598, 0.03043384892928801, ... |
708.2946 | The number of gauge singlets in supersymmetric Yang-Mills quantum
mechanics | We compute generating functions for number of U(N) (SU(N)) singlets in Fock
space in several space dimensions. The motivation to find the explicit form of
the functions is from the numerical approach to supersymmetric Yang-Mills
quantum mechanics, based on Fock space. Incidently the functions give many
important insi... | hep-th | we compute generating functions for number of un sun singlets in fock space in several space dimensions the motivation to find the explicit form of the functions is from the numerical approach to supersymmetric yangmills quantum mechanics based on fock space incidently the functions give many important insights into th... | [['we', 'compute', 'generating', 'functions', 'for', 'number', 'of', 'un', 'sun', 'singlets', 'in', 'fock', 'space', 'in', 'several', 'space', 'dimensions', 'the', 'motivation', 'to', 'find', 'the', 'explicit', 'form', 'of', 'the', 'functions', 'is', 'from', 'the', 'numerical', 'approach', 'to', 'supersymmetric', 'yang... | [-0.07031782752458464, 0.19721239846069039, -0.12329988730428006, 0.13618907731296004, -0.050525333634332606, -0.06915577742875668, -0.0253884921160837, 0.31489155751963455, -0.1759140859112928, -0.27058209867723154, 0.043165311699308324, -0.23071238678765663, -0.2246746419879951, 0.1874197954148577, -0.032827610770861... |
708.2947 | Detection of high-energy gamma rays from winter thunderclouds | A report is made on a comprehensive observation of a burst-like $\gamma$-ray
emission from thunderclouds on the Sea of Japan, during strong thunderstorms on
2007 January 6. The detected emission, lasting for $\sim$40 seconds, preceded
cloud-to-ground lightning discharges. The burst spectrum, extending to 10 MeV,
can ... | astro-ph physics.geo-ph | a report is made on a comprehensive observation of a burstlike gammaray emission from thunderclouds on the sea of japan during strong thunderstorms on 2007 january 6 the detected emission lasting for sim40 seconds preceded cloudtoground lightning discharges the burst spectrum extending to 10 mev can be interpreted as c... | [['a', 'report', 'is', 'made', 'on', 'a', 'comprehensive', 'observation', 'of', 'a', 'burstlike', 'gammaray', 'emission', 'from', 'thunderclouds', 'on', 'the', 'sea', 'of', 'japan', 'during', 'strong', 'thunderstorms', 'on', '2007', 'january', '6', 'the', 'detected', 'emission', 'lasting', 'for', 'sim40', 'seconds', 'p... | [-0.07937388877487844, 0.2555880563586582, -0.034615233465799214, 0.1140411705997439, -0.04361679769238963, -0.06734751919169485, 0.07015968843098776, 0.42843596099151504, -0.15320676018700957, -0.37984977483197496, 0.02469756582286209, -0.3310492205215089, 0.007719587672639776, 0.2564954520835553, -0.00949265980334193... |
708.2948 | Energy of knots and the infinitesimal cross ratio | This is a survey article on two topics. The Energy E of knots can be obtained
by generalizing an electrostatic energy of charged knots in order to produce
optimal knots. It turns out to be invariant under Moebius transformations. We
show that it can be expressed in terms of the infinitesimal cross ratio, which
is a c... | math.GT | this is a survey article on two topics the energy e of knots can be obtained by generalizing an electrostatic energy of charged knots in order to produce optimal knots it turns out to be invariant under moebius transformations we show that it can be expressed in terms of the infinitesimal cross ratio which is a conform... | [['this', 'is', 'a', 'survey', 'article', 'on', 'two', 'topics', 'the', 'energy', 'e', 'of', 'knots', 'can', 'be', 'obtained', 'by', 'generalizing', 'an', 'electrostatic', 'energy', 'of', 'charged', 'knots', 'in', 'order', 'to', 'produce', 'optimal', 'knots', 'it', 'turns', 'out', 'to', 'be', 'invariant', 'under', 'moe... | [-0.1928435051545071, 0.12291448436343881, -0.11748862992793035, 0.08395802863210869, -0.03284512902311503, -0.07164531817826895, -0.0322625065007462, 0.34084394540733254, -0.2605228553979825, -0.295018455825555, 0.048618155176369235, -0.25577342639175743, -0.13188634411646769, 0.19183345310963118, -0.04141251920746305... |
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