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 |
|---|---|---|---|---|---|---|
710.0353 | Trap-imbalanced fermion mixtures | We analyze the ground state phases of two-component ($\sigma \equiv \lbrace
\uparrow, \downarrow \rbrace$) population- and mass-balanced ($N_\uparrow =
N_\downarrow$ and $m_\uparrow = m_\downarrow$) but trap-imbalanced
($\omega_\uparrow \ne \omega_\downarrow$) fermion mixtures as a function of
interaction strength fr... | cond-mat.supr-con cond-mat.other | we analyze the ground state phases of twocomponent sigma equiv lbrace uparrow downarrow rbrace population and massbalanced n_uparrow n_downarrow and m_uparrow m_downarrow but trapimbalanced omega_uparrow ne omega_downarrow fermion mixtures as a function of interaction strength from the weak attraction bardeencooperschr... | [['we', 'analyze', 'the', 'ground', 'state', 'phases', 'of', 'twocomponent', 'sigma', 'equiv', 'lbrace', 'uparrow', 'downarrow', 'rbrace', 'population', 'and', 'massbalanced', 'n_uparrow', 'n_downarrow', 'and', 'm_uparrow', 'm_downarrow', 'but', 'trapimbalanced', 'omega_uparrow', 'ne', 'omega_downarrow', 'fermion', 'mi... | [-0.14704333916435847, 0.25018775765784085, -0.07067318700945988, 0.0692426065334412, 0.019518237455351348, -0.16796450091405185, 0.14292820547362445, 0.3177864971846618, -0.24378288704557, -0.18568468276687242, 0.005235899897309503, -0.3645887514231382, -0.012268935239666866, 0.050079175061977434, 0.07862502031353129,... |
710.0354 | The QCD Equation of State with almost Physical Quark Masses | We present results on the equation of state in QCD with two light quark
flavors and a heavier strange quark. Calculations with improved staggered
fermions have been performed on lattices with temporal extent Nt =4 and 6 on a
line of constant physics with almost physical quark mass values; the pion mass
is about 220 M... | hep-lat nucl-th | we present results on the equation of state in qcd with two light quark flavors and a heavier strange quark calculations with improved staggered fermions have been performed on lattices with temporal extent nt 4 and 6 on a line of constant physics with almost physical quark mass values the pion mass is about 220 mev an... | [['we', 'present', 'results', 'on', 'the', 'equation', 'of', 'state', 'in', 'qcd', 'with', 'two', 'light', 'quark', 'flavors', 'and', 'a', 'heavier', 'strange', 'quark', 'calculations', 'with', 'improved', 'staggered', 'fermions', 'have', 'been', 'performed', 'on', 'lattices', 'with', 'temporal', 'extent', 'nt', '4', '... | [-0.07902191400573384, 0.29186005757776623, -0.09399068525441491, 0.08699483996961356, -0.030584160321272865, -0.10832393927749519, 0.10985898771777568, 0.38719542551694847, -0.13651388784438917, -0.3063015948435882, 0.05613734970527996, -0.3165903544712176, 0.046480825465036235, 0.14439000230986715, 0.0814339550126843... |
710.0355 | A Simple Analytical Formulation for Periodic Orbits in Binary Stars | An analytical approximation to periodic orbits in the circular restricted
three-body problem is provided. The formulation given in this work is based in
calculations known from classical mechanics, but with the addition of the
necessary terms to give a fairly good approximation that we compare with
simulations, resul... | astro-ph | an analytical approximation to periodic orbits in the circular restricted threebody problem is provided the formulation given in this work is based in calculations known from classical mechanics but with the addition of the necessary terms to give a fairly good approximation that we compare with simulations resulting i... | [['an', 'analytical', 'approximation', 'to', 'periodic', 'orbits', 'in', 'the', 'circular', 'restricted', 'threebody', 'problem', 'is', 'provided', 'the', 'formulation', 'given', 'in', 'this', 'work', 'is', 'based', 'in', 'calculations', 'known', 'from', 'classical', 'mechanics', 'but', 'with', 'the', 'addition', 'of',... | [-0.13444333150672416, 0.020585265353826494, -0.10650614323715368, 0.04513999061814199, -0.06295935407280923, -0.09183711644262076, 0.041800397265081606, 0.33052755968024333, -0.22265074624990425, -0.2982301589970787, 0.08578032128047199, -0.22836540506531794, -0.1768772457788388, 0.23468961811624467, -0.05080339642862... |
710.0356 | Mapping the geometry of the E6 group | In this paper we present a construction for the compact form of the
exceptional Lie group E6 by exponentiating the corresponding Lie algebra e6,
which we realize as the the sum of f4, the derivations of the exceptional
Jordan algebra J3 of dimension 3 with octonionic entries, and the right
multiplication by the eleme... | math-ph hep-th math.MP | in this paper we present a construction for the compact form of the exceptional lie group e6 by exponentiating the corresponding lie algebra e6 which we realize as the the sum of f4 the derivations of the exceptional jordan algebra j3 of dimension 3 with octonionic entries and the right multiplication by the elements o... | [['in', 'this', 'paper', 'we', 'present', 'a', 'construction', 'for', 'the', 'compact', 'form', 'of', 'the', 'exceptional', 'lie', 'group', 'e6', 'by', 'exponentiating', 'the', 'corresponding', 'lie', 'algebra', 'e6', 'which', 'we', 'realize', 'as', 'the', 'the', 'sum', 'of', 'f4', 'the', 'derivations', 'of', 'the', 'e... | [-0.14440185190037344, 0.05209375403677713, -0.06317691947509901, 0.02779744773358812, -0.12104770444531107, -0.10936688029941058, 0.015893699877338033, 0.3621546225904515, -0.21758605512987936, -0.23764618922106104, 0.13944303655421897, -0.22915193667116304, -0.17250841201254816, 0.1818018327220202, -0.078688991333668... |
710.0357 | On Floer homology and the Berge conjecture on knots admitting lens space
surgeries | We complete the first step in a two-part program proposed by Baker, Grigsby,
and the author to prove that Berge's construction of knots in the three-sphere
which admit lens space surgeries is complete. The first step, which we prove
here, is to show that a knot in a lens space with a three-sphere surgery has
simple (... | math.GT math.SG | we complete the first step in a twopart program proposed by baker grigsby and the author to prove that berges construction of knots in the threesphere which admit lens space surgeries is complete the first step which we prove here is to show that a knot in a lens space with a threesphere surgery has simple in the sense... | [['we', 'complete', 'the', 'first', 'step', 'in', 'a', 'twopart', 'program', 'proposed', 'by', 'baker', 'grigsby', 'and', 'the', 'author', 'to', 'prove', 'that', 'berges', 'construction', 'of', 'knots', 'in', 'the', 'threesphere', 'which', 'admit', 'lens', 'space', 'surgeries', 'is', 'complete', 'the', 'first', 'step',... | [-0.21767887992163498, 0.033642388411487145, -0.17137755264838536, 0.06567404244250308, -0.10490663561814775, -0.17264775011998912, 0.0009156396783267458, 0.34911041530470055, -0.2428586119506508, -0.2984085378050804, 0.08856973646519085, -0.1825623274408281, -0.22592799353878945, 0.19106457149609923, -0.14114806894523... |
710.0358 | Friedel oscillations in one-dimensional metals: from Luttinger's theorem
to the Luttinger liquid | Charge density and magnetization density profiles of one-dimensional metals
are investigated by two complementary many-body methods: numerically exact
(Lanczos) diagonalization, and the Bethe-Ansatz local-density approximation
with and without a simple self-interaction correction. Depending on the
magnetization of th... | cond-mat.str-el cond-mat.mtrl-sci | charge density and magnetization density profiles of onedimensional metals are investigated by two complementary manybody methods numerically exact lanczos diagonalization and the betheansatz localdensity approximation with and without a simple selfinteraction correction depending on the magnetization of the system loc... | [['charge', 'density', 'and', 'magnetization', 'density', 'profiles', 'of', 'onedimensional', 'metals', 'are', 'investigated', 'by', 'two', 'complementary', 'manybody', 'methods', 'numerically', 'exact', 'lanczos', 'diagonalization', 'and', 'the', 'betheansatz', 'localdensity', 'approximation', 'with', 'and', 'without'... | [-0.14801747273653745, 0.09991808593273163, -0.10901464151218533, 0.1182184368930757, 0.012020263224840164, -0.17539811138994993, 0.05650765299797058, 0.3531402693875134, -0.23350804135203362, -0.2565658934263047, 0.008876085057854652, -0.32636673534289, -0.10525185383812641, 0.15083541054278612, 0.14469087908044456, 0... |
710.0359 | Grid Diagrams for Lens Spaces and Combinatorial Knot Floer Homology | Similar to knots in S^3, any knot in a lens space has a grid diagram from
which one can combinatorially compute all of its knot Floer homology
invariants. We give an explicit description of the generators, differentials,
and rational Maslov and Alexander gradings in terms of combinatorial data on
the grid diagram. Mo... | math.GT math.SG | similar to knots in s3 any knot in a lens space has a grid diagram from which one can combinatorially compute all of its knot floer homology invariants we give an explicit description of the generators differentials and rational maslov and alexander gradings in terms of combinatorial data on the grid diagram motivated ... | [['similar', 'to', 'knots', 'in', 's3', 'any', 'knot', 'in', 'a', 'lens', 'space', 'has', 'a', 'grid', 'diagram', 'from', 'which', 'one', 'can', 'combinatorially', 'compute', 'all', 'of', 'its', 'knot', 'floer', 'homology', 'invariants', 'we', 'give', 'an', 'explicit', 'description', 'of', 'the', 'generators', 'differe... | [-0.2712515710741776, 0.023579836697616426, -0.15031017691094792, 0.10216706947514177, -0.12037391383283302, -0.15823036414134292, -0.009676112919073322, 0.33589222830250465, -0.27574374136078145, -0.34575062507219545, 0.083019957134904, -0.23390981238500208, -0.19504028164773388, 0.16095484002489202, -0.20257884802593... |
710.036 | Interpolation in Valiant's theory | We investigate the following question: if a polynomial can be evaluated at
rational points by a polynomial-time boolean algorithm, does it have a
polynomial-size arithmetic circuit? We argue that this question is certainly
difficult. Answering it negatively would indeed imply that the constant-free
versions of the al... | cs.CC | we investigate the following question if a polynomial can be evaluated at rational points by a polynomialtime boolean algorithm does it have a polynomialsize arithmetic circuit we argue that this question is certainly difficult answering it negatively would indeed imply that the constantfree versions of the algebraic c... | [['we', 'investigate', 'the', 'following', 'question', 'if', 'a', 'polynomial', 'can', 'be', 'evaluated', 'at', 'rational', 'points', 'by', 'a', 'polynomialtime', 'boolean', 'algorithm', 'does', 'it', 'have', 'a', 'polynomialsize', 'arithmetic', 'circuit', 'we', 'argue', 'that', 'this', 'question', 'is', 'certainly', '... | [-0.12338816529715897, 0.04324378945800473, -0.09238936903084376, 0.12750899972194923, -0.0867935490385344, -0.1755732262770866, 0.07726538065024194, 0.32375342769661347, -0.3212528970157135, -0.3051476392523531, 0.09813130489682423, -0.19458892497885433, -0.1716152989235572, 0.24110096205171264, -0.12182665473328651, ... |
710.0361 | Monolithic Pixels R&D at LBNL | This paper reports recent results from the ongoing R&D on monolithic pixels
for the ILC Vertex Tracker at LBNL.
| physics.ins-det | this paper reports recent results from the ongoing rd on monolithic pixels for the ilc vertex tracker at lbnl | [['this', 'paper', 'reports', 'recent', 'results', 'from', 'the', 'ongoing', 'rd', 'on', 'monolithic', 'pixels', 'for', 'the', 'ilc', 'vertex', 'tracker', 'at', 'lbnl']] | [0.022166236548831587, 0.06642466741859128, -0.007356046282343175, -0.15310361347234758, -0.05548312637562815, -0.0758958876525101, -0.04647620850071115, 0.4098276613574279, -0.15036199408534326, -0.2445866681243244, 0.10572460234949463, -0.44871536426638303, -0.06828331986540243, 0.19148377799674085, -0.10151860328685... |
710.0362 | Spontaneous P-parity violation in dense baryon matter | We investigate possibilities for dynamical P-parity violation in dense baryon
matter in the framework of effective quark models. Dynamical P-parity violation
can appear in models with at least two scalar and two pseudoscalar fields,
where both scalar fields are condensed at normal conditions. At special
configuration... | hep-ph | we investigate possibilities for dynamical pparity violation in dense baryon matter in the framework of effective quark models dynamical pparity violation can appear in models with at least two scalar and two pseudoscalar fields where both scalar fields are condensed at normal conditions at special configurations of co... | [['we', 'investigate', 'possibilities', 'for', 'dynamical', 'pparity', 'violation', 'in', 'dense', 'baryon', 'matter', 'in', 'the', 'framework', 'of', 'effective', 'quark', 'models', 'dynamical', 'pparity', 'violation', 'can', 'appear', 'in', 'models', 'with', 'at', 'least', 'two', 'scalar', 'and', 'two', 'pseudoscalar... | [-0.16721055348792557, 0.303700387138801, -0.06192602037318792, 0.11421735850569692, -0.07299216923719833, -0.1468695605431403, 0.016983798644008133, 0.2738989195017849, -0.20798104344098603, -0.28833101897328656, 0.010334057627173448, -0.2805472164374134, -0.06606284111231855, 0.12054447840573718, 0.09484427954856921,... |
710.0363 | Central limits and homogenization in random media | We consider the perturbation of elliptic operators of the form
$P(\bx,\bD)$ by random, rapidly varying, sufficiently mixing, potentials of
the form $q(\frac{\bx}\eps,\omega)$. We analyze the source and spectral
problems associated to such operators and show that the properly renormalized
difference between the pert... | math.AP math.PR | we consider the perturbation of elliptic operators of the form pbxbd by random rapidly varying sufficiently mixing potentials of the form qfracbxepsomega we analyze the source and spectral problems associated to such operators and show that the properly renormalized difference between the perturbed and unperturbed solu... | [['we', 'consider', 'the', 'perturbation', 'of', 'elliptic', 'operators', 'of', 'the', 'form', 'pbxbd', 'by', 'random', 'rapidly', 'varying', 'sufficiently', 'mixing', 'potentials', 'of', 'the', 'form', 'qfracbxepsomega', 'we', 'analyze', 'the', 'source', 'and', 'spectral', 'problems', 'associated', 'to', 'such', 'oper... | [-0.11071127028326835, 0.13262795865283175, -0.07597247609016249, 0.10314219397889123, -0.024346926476474913, -0.10650267173788684, -0.0022478198674033886, 0.3116791818953924, -0.27181564587941864, -0.2559482241522963, 0.16891087614536537, -0.3015086478751026, -0.12688682706616186, 0.22659305274739103, -0.0484718782551... |
710.0364 | Modified Gravity: Cosmology without dark matter or Einstein's
cosmological constant | We explore the cosmological consequences of Modified Gravity (MOG), and find
that it provides, using a minimal number of parameters, good fits to data,
including CMB temperature anisotropy, galaxy power spectrum, and supernova
luminosity-distance observations without exotic dark matter. MOG predicts a
bouncing cosmol... | astro-ph gr-qc | we explore the cosmological consequences of modified gravity mog and find that it provides using a minimal number of parameters good fits to data including cmb temperature anisotropy galaxy power spectrum and supernova luminositydistance observations without exotic dark matter mog predicts a bouncing cosmology with a v... | [['we', 'explore', 'the', 'cosmological', 'consequences', 'of', 'modified', 'gravity', 'mog', 'and', 'find', 'that', 'it', 'provides', 'using', 'a', 'minimal', 'number', 'of', 'parameters', 'good', 'fits', 'to', 'data', 'including', 'cmb', 'temperature', 'anisotropy', 'galaxy', 'power', 'spectrum', 'and', 'supernova', ... | [-0.10382857339767118, 0.10814111342406249, -0.150170054154781, 0.13741515188788375, -0.16305193662022552, -0.14086659877405813, -0.04930097192215423, 0.31471230326375615, -0.17666881874514123, -0.4026256900901596, -0.002987334760837257, -0.2835033881710842, -0.017998197674751283, 0.21048971532533567, 0.023609919007867... |
710.0365 | Large oscillating non-local voltage in multi-terminal single wall carbon
nanotube devices | We report on the observation of a non-local voltage in a ballistic
one-dimensional conductor, realized by a single-wall carbon nanotube with four
contacts. The contacts divide the tube into three quantum dots which we control
by the back-gate voltage $V_g$. We measure a large \emph{oscillating} non-local
voltage $V_{... | cond-mat.mes-hall | we report on the observation of a nonlocal voltage in a ballistic onedimensional conductor realized by a singlewall carbon nanotube with four contacts the contacts divide the tube into three quantum dots which we control by the backgate voltage v_g we measure a large emphoscillating nonlocal voltage v_nl as a function ... | [['we', 'report', 'on', 'the', 'observation', 'of', 'a', 'nonlocal', 'voltage', 'in', 'a', 'ballistic', 'onedimensional', 'conductor', 'realized', 'by', 'a', 'singlewall', 'carbon', 'nanotube', 'with', 'four', 'contacts', 'the', 'contacts', 'divide', 'the', 'tube', 'into', 'three', 'quantum', 'dots', 'which', 'we', 'co... | [-0.1865843304231302, 0.1589446096517837, -0.062280563134748064, 0.007178508567374162, -0.005688144623772385, -0.21075134093095502, 0.07352352278431896, 0.3808143673099808, -0.27058136280741274, -0.30558010275216446, 0.027923152858833063, -0.2818951564360909, -0.11605423959644184, 0.20407793576980354, -0.05439670013561... |
710.0366 | Coupling constant constraints in a nonminimally coupled phantom
cosmology | In the paper we investigate observational constraints on coupling to gravity
constant parameter $\xi$ using distant supernovae SNIa data, baryon oscillation
peak (BOP), the cosmic microwave background radiation (CMBR) shift parameter,
and $H(z)$ data set. We estimate the value of this parameter to constrain the
exten... | astro-ph gr-qc hep-th | in the paper we investigate observational constraints on coupling to gravity constant parameter xi using distant supernovae snia data baryon oscillation peak bop the cosmic microwave background radiation cmbr shift parameter and hz data set we estimate the value of this parameter to constrain the extended quintessence ... | [['in', 'the', 'paper', 'we', 'investigate', 'observational', 'constraints', 'on', 'coupling', 'to', 'gravity', 'constant', 'parameter', 'xi', 'using', 'distant', 'supernovae', 'snia', 'data', 'baryon', 'oscillation', 'peak', 'bop', 'the', 'cosmic', 'microwave', 'background', 'radiation', 'cmbr', 'shift', 'parameter', ... | [-0.14383949854120773, 0.13354334833979187, -0.044097614144125295, 0.11197543544544568, -0.18761253668813996, -0.15900458079031718, 0.05090120542038392, 0.2768007924640051, -0.20672345345699658, -0.3335352671002188, 0.022111916231111653, -0.3172753973393351, -0.01758076840202995, 0.1813892846881983, 0.02514105512232016... |
710.0367 | Discovery of an X-ray nebula around PSR J1718-3825 and implications for
the nature of the gamma-ray source HESS J1718-385 | Combined X-ray synchrotron and inverse-Compton gamma-ray observations of
pulsar wind nebulae (PWN) may help to elucidate the processes of acceleration
and energy loss in these systems. In particular, such observations provide
constraints on the particle injection history and the magnetic field strength
in these objec... | astro-ph | combined xray synchrotron and inversecompton gammaray observations of pulsar wind nebulae pwn may help to elucidate the processes of acceleration and energy loss in these systems in particular such observations provide constraints on the particle injection history and the magnetic field strength in these objects the ne... | [['combined', 'xray', 'synchrotron', 'and', 'inversecompton', 'gammaray', 'observations', 'of', 'pulsar', 'wind', 'nebulae', 'pwn', 'may', 'help', 'to', 'elucidate', 'the', 'processes', 'of', 'acceleration', 'and', 'energy', 'loss', 'in', 'these', 'systems', 'in', 'particular', 'such', 'observations', 'provide', 'const... | [-0.07379117061556253, 0.09471521467570063, -0.04348425771594558, 0.1449188873417395, -0.16372479058878675, -0.05348284826741541, 0.048451102726250785, 0.4454887919127941, -0.2121598722065531, -0.3718316724957669, 0.05464829564132817, -0.32132106953721545, 0.031353503912176985, 0.2671656290552426, 0.014865944355571554,... |
710.0368 | The electronic bands of CrD, CrH, MgD and MgH: application to the
"deuterium test" | We compute opacities for the electronic molecular band systems A 6Sigma+ -- X
6Sigma+ of CrH and CrD, and A 2Pi -- X 2Sigma+ of MgH and MgD. The opacities
are computed by making use of existing spectroscopic constants for MgH and CrH.
These constants are adjusted for the different reduced masses of MgD and CrD.
Frank... | astro-ph | we compute opacities for the electronic molecular band systems a 6sigma x 6sigma of crh and crd and a 2pi x 2sigma of mgh and mgd the opacities are computed by making use of existing spectroscopic constants for mgh and crh these constants are adjusted for the different reduced masses of mgd and crd frankcondon factors ... | [['we', 'compute', 'opacities', 'for', 'the', 'electronic', 'molecular', 'band', 'systems', 'a', '6sigma', 'x', '6sigma', 'of', 'crh', 'and', 'crd', 'and', 'a', '2pi', 'x', '2sigma', 'of', 'mgh', 'and', 'mgd', 'the', 'opacities', 'are', 'computed', 'by', 'making', 'use', 'of', 'existing', 'spectroscopic', 'constants', ... | [-0.05278227359016646, 0.11017777712865943, -0.005090832907865804, 0.07301626921329635, -0.016107679277315344, -0.12694490225495478, 0.09678140103718952, 0.4093952121789028, -0.19005305248107393, -0.3409711951022281, 0.018409043473136415, -0.28131929293005287, -0.057161204544459714, 0.22159334524277305, -0.005062346790... |
710.0369 | Thermodynamics of Ion Solvation and Differential Adsorption at
Liquid-Liquid Interfaces and Membranes | We construct a mean-field formulation of the thermodynamics of ion solvation
in immiscible polar binary mixtures. Assuming an equilibrium planar interface
separating two semi-infinite regions of different constant dielectric medium,
we study the electrostatic phenomenon of differential adsorption of ions at the
inter... | cond-mat.soft cond-mat.mtrl-sci | we construct a meanfield formulation of the thermodynamics of ion solvation in immiscible polar binary mixtures assuming an equilibrium planar interface separating two semiinfinite regions of different constant dielectric medium we study the electrostatic phenomenon of differential adsorption of ions at the interface u... | [['we', 'construct', 'a', 'meanfield', 'formulation', 'of', 'the', 'thermodynamics', 'of', 'ion', 'solvation', 'in', 'immiscible', 'polar', 'binary', 'mixtures', 'assuming', 'an', 'equilibrium', 'planar', 'interface', 'separating', 'two', 'semiinfinite', 'regions', 'of', 'different', 'constant', 'dielectric', 'medium',... | [-0.12223644123687485, 0.1758245120121292, -0.04817164200358093, 0.03606739477159028, 0.023989336004053226, -0.15357372047547557, 0.030331966329793462, 0.39666297352399493, -0.2834258825731937, -0.26572449166388784, -0.01596997967314311, -0.28269135793212985, -0.1066433004615065, 0.08777683587615058, 0.0287470583666543... |
710.037 | MegaPipe: the MegaCam image stacking pipeline at the Canadian
Astronomical Data Centre | This paper describes the MegaPipe image processing pipeline at the Canadian
Astronomical Data Centre. The pipeline combines multiple images from the
MegaCam mosaic camera on CFHT and combines them into a single output image.
MegaPipe takes as input detrended MegaCam images and does a careful astrometric
and photometr... | astro-ph | this paper describes the megapipe image processing pipeline at the canadian astronomical data centre the pipeline combines multiple images from the megacam mosaic camera on cfht and combines them into a single output image megapipe takes as input detrended megacam images and does a careful astrometric and photometric c... | [['this', 'paper', 'describes', 'the', 'megapipe', 'image', 'processing', 'pipeline', 'at', 'the', 'canadian', 'astronomical', 'data', 'centre', 'the', 'pipeline', 'combines', 'multiple', 'images', 'from', 'the', 'megacam', 'mosaic', 'camera', 'on', 'cfht', 'and', 'combines', 'them', 'into', 'a', 'single', 'output', 'i... | [-0.025474396269095853, -0.03012974712031859, -0.140233877377964, 0.050543158842224836, -0.1143903902783576, -0.10596745030488819, 0.03208666074378588, 0.4980558046243257, -0.25639577718296397, -0.39089030990618523, 0.10045137592155866, -0.3725583524684663, -0.00924250488040141, 0.219852019480809, -0.1697373027973636, ... |
710.0371 | Lyman-alpha Damping Wing Constraints on Inhomogeneous Reionization | One well-known way to constrain the hydrogen neutral fraction, x_H, of the
high-redshift intergalactic medium (IGM) is through the shape of the red
damping wing of the Lya absorption line. We examine this method's effectiveness
in light of recent models showing that the IGM neutral fraction is highly
inhomogeneous on... | astro-ph | one wellknown way to constrain the hydrogen neutral fraction x_h of the highredshift intergalactic medium igm is through the shape of the red damping wing of the lya absorption line we examine this methods effectiveness in light of recent models showing that the igm neutral fraction is highly inhomogeneous on large sca... | [['one', 'wellknown', 'way', 'to', 'constrain', 'the', 'hydrogen', 'neutral', 'fraction', 'x_h', 'of', 'the', 'highredshift', 'intergalactic', 'medium', 'igm', 'is', 'through', 'the', 'shape', 'of', 'the', 'red', 'damping', 'wing', 'of', 'the', 'lya', 'absorption', 'line', 'we', 'examine', 'this', 'methods', 'effective... | [-0.03887406818982628, 0.13145562209188938, -0.052313515927849545, 0.10546940500485814, -0.10514677998816802, -0.09287955799450477, 0.01720093976162995, 0.4231997624743316, -0.19853944265180165, -0.3088003356444339, 0.04737557736949788, -0.2870195481719242, -0.04648858374812537, 0.17502958538321156, -0.0124992020407484... |
710.0372 | The Revealing Dust: Mid-Infrared Activity in Hickson Compact Group
Galaxy Nuclei | We present a sample of 46 galaxy nuclei from 12 nearby (z<4500 km/s) Hickson
Compact Groups (HCGs) with a complete suite of 1-24 micron 2MASS+Spitzer
nuclear photometry. For all objects in the sample, blue emission from stellar
photospheres dominates in the near-IR through the 3.6 micron IRAC band.
Twenty-five of 46 ... | astro-ph | we present a sample of 46 galaxy nuclei from 12 nearby z4500 kms hickson compact groups hcgs with a complete suite of 124 micron 2massspitzer nuclear photometry for all objects in the sample blue emission from stellar photospheres dominates in the nearir through the 36 micron irac band twentyfive of 46 54 galaxy nuclei... | [['we', 'present', 'a', 'sample', 'of', '46', 'galaxy', 'nuclei', 'from', '12', 'nearby', 'z4500', 'kms', 'hickson', 'compact', 'groups', 'hcgs', 'with', 'a', 'complete', 'suite', 'of', '124', 'micron', '2massspitzer', 'nuclear', 'photometry', 'for', 'all', 'objects', 'in', 'the', 'sample', 'blue', 'emission', 'from', ... | [-0.0027539898800392594, 0.08927596511051915, -0.07277472721371077, 0.10139784519169688, -0.07053406751686846, -0.061329166680086165, 0.07105181916267611, 0.4824979599572218, -0.12011487477584117, -0.3606296200131469, 0.025806510601620147, -0.3266473842590158, -0.018990636353186374, 0.1949049562090702, -0.0435519621298... |
710.0373 | To Bin or Not To Bin: Decorrelating the Cosmic Equation of State | The physics behind the acceleration of the cosmic expansion can be elucidated
through comparison of the predictions of dark energy equations of state to
observational data. In seeking to optimize this, we investigate the advantages
and disadvantages of using principal component analysis, uncorrelated
bandpowers, and ... | astro-ph | the physics behind the acceleration of the cosmic expansion can be elucidated through comparison of the predictions of dark energy equations of state to observational data in seeking to optimize this we investigate the advantages and disadvantages of using principal component analysis uncorrelated bandpowers and the eq... | [['the', 'physics', 'behind', 'the', 'acceleration', 'of', 'the', 'cosmic', 'expansion', 'can', 'be', 'elucidated', 'through', 'comparison', 'of', 'the', 'predictions', 'of', 'dark', 'energy', 'equations', 'of', 'state', 'to', 'observational', 'data', 'in', 'seeking', 'to', 'optimize', 'this', 'we', 'investigate', 'the... | [-0.07258530073786376, 0.05359864302210236, -0.12044365812571498, 0.0635213915540606, -0.10877841885346885, -0.08355971046407289, 0.0475465842531225, 0.36389635236711676, -0.2557200301893017, -0.34364043206079015, 0.07990940240982902, -0.286158682475157, -0.081566550459183, 0.18756562736047722, 0.010197015229287908, 0.... |
710.0374 | A chiral cascade via backreacting D7-branes with flux | In the context of AdS/CFT, we consider a cascading theory with an arbitrarily
large number of chiral flavors. In the UV the theory can be considered as a
chiral flavoring of the Klebanov-Tseytlin solution, and exhibits a duality
wall. Instead in the IR, due to the rich dynamics, it safely flows to a
non-cascading the... | hep-th | in the context of adscft we consider a cascading theory with an arbitrarily large number of chiral flavors in the uv the theory can be considered as a chiral flavoring of the klebanovtseytlin solution and exhibits a duality wall instead in the ir due to the rich dynamics it safely flows to a noncascading theory we engi... | [['in', 'the', 'context', 'of', 'adscft', 'we', 'consider', 'a', 'cascading', 'theory', 'with', 'an', 'arbitrarily', 'large', 'number', 'of', 'chiral', 'flavors', 'in', 'the', 'uv', 'the', 'theory', 'can', 'be', 'considered', 'as', 'a', 'chiral', 'flavoring', 'of', 'the', 'klebanovtseytlin', 'solution', 'and', 'exhibit... | [-0.15721691569577403, 0.1678259669655043, -0.07160680725580214, 0.08339844099942624, -0.0693419300254405, -0.14620290058994972, 0.01207728416559939, 0.2922115512907241, -0.16607711075504464, -0.2823609284053769, 0.08141878528766129, -0.2875524052367436, -0.15094892775289728, 0.05160919738214786, -0.09317144841060233, ... |
710.0375 | Spider Optimization: Probing the Systematics of a Large Scale B-Mode
Experiment | Spider is a long-duration, balloon-borne polarimeter designed to measure
large scale Cosmic Microwave Background (CMB) polarization with very high
sensitivity and control of systematics. The instrument will map over half the
sky with degree angular resolution in I, Q and U Stokes parameters, in four
frequency bands f... | astro-ph | spider is a longduration balloonborne polarimeter designed to measure large scale cosmic microwave background cmb polarization with very high sensitivity and control of systematics the instrument will map over half the sky with degree angular resolution in i q and u stokes parameters in four frequency bands from 96 to ... | [['spider', 'is', 'a', 'longduration', 'balloonborne', 'polarimeter', 'designed', 'to', 'measure', 'large', 'scale', 'cosmic', 'microwave', 'background', 'cmb', 'polarization', 'with', 'very', 'high', 'sensitivity', 'and', 'control', 'of', 'systematics', 'the', 'instrument', 'will', 'map', 'over', 'half', 'the', 'sky',... | [-0.1601182573204008, 0.1617085358767636, -0.05053607305060573, 0.024096945890575917, -0.1028209327403264, -0.1315379907945939, 0.00046780492843983255, 0.4065193917275858, -0.2480116765082036, -0.333895501200609, 0.0999899501396228, -0.29068194468476877, -0.061726108444230536, 0.2287847658561677, -0.06142112733940258, ... |
710.0376 | Equivalence of QCD in the epsilon-regime and chiral Random Matrix Theory
with or without chemical potential | We prove that QCD in the epsilon-regime of chiral Perturbation Theory is
equivalent to chiral Random Matrix Theory for zero and both non-zero real and
imaginary chemical potential mu. To this aim we prove a theorem that relates
integrals over fermionic and bosonic variables to super-Hermitian or
super-Unitary groups ... | hep-th hep-lat math-ph math.MP | we prove that qcd in the epsilonregime of chiral perturbation theory is equivalent to chiral random matrix theory for zero and both nonzero real and imaginary chemical potential mu to this aim we prove a theorem that relates integrals over fermionic and bosonic variables to superhermitian or superunitary groups also ca... | [['we', 'prove', 'that', 'qcd', 'in', 'the', 'epsilonregime', 'of', 'chiral', 'perturbation', 'theory', 'is', 'equivalent', 'to', 'chiral', 'random', 'matrix', 'theory', 'for', 'zero', 'and', 'both', 'nonzero', 'real', 'and', 'imaginary', 'chemical', 'potential', 'mu', 'to', 'this', 'aim', 'we', 'prove', 'a', 'theorem'... | [-0.12859324840828776, 0.21398227070935535, -0.10535906236246229, 0.09554409767966718, -0.04083423154242337, -0.10622318190708756, 0.04022291866503656, 0.36185663460195067, -0.18789181958884002, -0.20246688463166357, 0.03989664686657488, -0.29485111743584275, -0.1334421727564186, 0.10286403838731349, 0.0251649713888764... |
710.0377 | Idempotent and tropical mathematics and problems of mathematical physics
(Volume I) | This volume contains the proceedings of an International Workshop on
Idempotent and Tropical Mathematics and Problems of Mathematical Physics, held
at the Independent University of Moscow, Russia, on August 25-30, 2007.
| math.RA math-ph math.AG math.AP math.MP math.OA math.OC math.RT | this volume contains the proceedings of an international workshop on idempotent and tropical mathematics and problems of mathematical physics held at the independent university of moscow russia on august 2530 2007 | [['this', 'volume', 'contains', 'the', 'proceedings', 'of', 'an', 'international', 'workshop', 'on', 'idempotent', 'and', 'tropical', 'mathematics', 'and', 'problems', 'of', 'mathematical', 'physics', 'held', 'at', 'the', 'independent', 'university', 'of', 'moscow', 'russia', 'on', 'august', '2530', '2007']] | [-0.011629003730993117, 0.12600010305487236, -0.1050400729291141, -0.014012984439520346, -0.07583430169090148, -0.03690992935650771, 0.012907107030191729, 0.1485545088747336, -0.20300530709867035, -0.403802098225682, 0.19190950150932035, -0.3740427882050074, -0.09267368732440856, 0.22756542529790633, -0.205881797918869... |
710.0378 | Inflated planets and their low-mass companions | Various mechanisms have been proposed to explain the inflated size of HD
209458b after it became clear that it has no companions capable of producing a
stellar reflex velocity greater than around 5 m/s. Had there been such a
companion, the hypothesis that it forces the eccentricity of the inflated
planet thereby tida... | astro-ph | various mechanisms have been proposed to explain the inflated size of hd 209458b after it became clear that it has no companions capable of producing a stellar reflex velocity greater than around 5 ms had there been such a companion the hypothesis that it forces the eccentricity of the inflated planet thereby tidally h... | [['various', 'mechanisms', 'have', 'been', 'proposed', 'to', 'explain', 'the', 'inflated', 'size', 'of', 'hd', '209458b', 'after', 'it', 'became', 'clear', 'that', 'it', 'has', 'no', 'companions', 'capable', 'of', 'producing', 'a', 'stellar', 'reflex', 'velocity', 'greater', 'than', 'around', '5', 'ms', 'had', 'there',... | [-0.1064930312766307, 0.1972945990718206, -0.08659549045129394, 0.06355353674998511, -0.12148190585763327, -0.08519234959999113, 0.04739237004070587, 0.3733865545657115, -0.1299187592624728, -0.3663604685143397, 0.08756071445294561, -0.2684474627481026, -0.09089159010434333, 0.23492478068639228, -0.11947455334154014, 0... |
710.0379 | Consistent estimates of deformed isotropic Gaussian random fields on the
plane | This paper proves fixed domain asymptotic results for estimating a smooth
invertible transformation $f:\Bbb{R}^2\to\Bbb{R}^2$ when observing the deformed
random field $Z\circ f$ on a dense grid in a bounded, simply connected domain
$\Omega$, where $Z$ is assumed to be an isotropic Gaussian random field on
$\Bbb{R}^2$... | math.ST stat.TH | this paper proves fixed domain asymptotic results for estimating a smooth invertible transformation fbbbr2tobbbr2 when observing the deformed random field zcirc f on a dense grid in a bounded simply connected domain omega where z is assumed to be an isotropic gaussian random field on bbbr2 the estimate hatf is construc... | [['this', 'paper', 'proves', 'fixed', 'domain', 'asymptotic', 'results', 'for', 'estimating', 'a', 'smooth', 'invertible', 'transformation', 'fbbbr2tobbbr2', 'when', 'observing', 'the', 'deformed', 'random', 'field', 'zcirc', 'f', 'on', 'a', 'dense', 'grid', 'in', 'a', 'bounded', 'simply', 'connected', 'domain', 'omega... | [-0.13589401758154449, 0.12792023692378754, -0.05728504034569082, 0.020692312255825684, -0.08900611203204355, -0.13981224275801493, 0.02969890153237983, 0.40508188062711903, -0.3100904558663783, -0.15830390342187298, 0.13147497593283491, -0.24715915179770925, -0.11528581046630912, 0.18011710899274636, -0.11980756802646... |
710.038 | Fluctuations of particle ratios as a freeze-out probe | We explain how event-by-event fluctuations of particle ratios can constrain
and falsify the statistical model of particle production in heavy ion
collisions, using $K/\pi$ fluctuations as an example. We define an observable
capable of determining which statistical model, if any, governs freeze-out in
ultrarelativisti... | nucl-th | we explain how eventbyevent fluctuations of particle ratios can constrain and falsify the statistical model of particle production in heavy ion collisions using kpi fluctuations as an example we define an observable capable of determining which statistical model if any governs freezeout in ultrarelativistic heavy ion c... | [['we', 'explain', 'how', 'eventbyevent', 'fluctuations', 'of', 'particle', 'ratios', 'can', 'constrain', 'and', 'falsify', 'the', 'statistical', 'model', 'of', 'particle', 'production', 'in', 'heavy', 'ion', 'collisions', 'using', 'kpi', 'fluctuations', 'as', 'an', 'example', 'we', 'define', 'an', 'observable', 'capab... | [-0.042741813863174126, 0.27520123354556475, -0.18421100767852824, 0.15368770671250553, 0.015687164966187446, -0.13549085056981425, -0.002148810895829419, 0.2875364421945966, -0.23797020200469526, -0.2733313324891664, -0.040934445134826684, -0.30241759015502884, 0.002420392365261815, 0.1122116839622655, 0.0220782294644... |
710.0381 | The galaxy stellar mass-star formation rate relation: Evidence for an
evolving stellar initial mass function? | The evolution of the galaxy stellar mass--star formation rate relationship
(M*-SFR) provides key constraints on the stellar mass assembly histories of
galaxies. For star-forming galaxies, M*-SFR is observed to be fairly tight with
a slope close to unity from z~0-2. Simulations of galaxy formation reproduce
these tren... | astro-ph | the evolution of the galaxy stellar massstar formation rate relationship msfr provides key constraints on the stellar mass assembly histories of galaxies for starforming galaxies msfr is observed to be fairly tight with a slope close to unity from z02 simulations of galaxy formation reproduce these trends owing to the ... | [['the', 'evolution', 'of', 'the', 'galaxy', 'stellar', 'massstar', 'formation', 'rate', 'relationship', 'msfr', 'provides', 'key', 'constraints', 'on', 'the', 'stellar', 'mass', 'assembly', 'histories', 'of', 'galaxies', 'for', 'starforming', 'galaxies', 'msfr', 'is', 'observed', 'to', 'be', 'fairly', 'tight', 'with',... | [-0.05783958854440171, 0.13185225759673538, -0.09831360495041332, 0.157476903076583, -0.08820050500891363, -0.07912949480242022, 0.04411100185040148, 0.40784194803101914, -0.1496052797588091, -0.37405672713020255, 0.0011835199243034281, -0.25403380268696873, -0.04003226351735412, 0.18372008846037918, -0.035645004125088... |
710.0382 | The Suzaku Observation of NGC 3516: Complex Absorption and the Broad and
Narrow Fe K Lines | We present results from a 150 ksec Suzaku observation of the Seyfert 1.5 NGC
3516 in October 2005. The source was in a relatively highly absorbed state. Our
best-fit model is consistent with the presence of a low-ionization absorber
which has a column density near 5 * 10^{22} cm^{-2} and covers most of the
X-ray cont... | astro-ph | we present results from a 150 ksec suzaku observation of the seyfert 15 ngc 3516 in october 2005 the source was in a relatively highly absorbed state our bestfit model is consistent with the presence of a lowionization absorber which has a column density near 5 1022 cm2 and covers most of the xray continuum source cove... | [['we', 'present', 'results', 'from', 'a', '150', 'ksec', 'suzaku', 'observation', 'of', 'the', 'seyfert', '15', 'ngc', '3516', 'in', 'october', '2005', 'the', 'source', 'was', 'in', 'a', 'relatively', 'highly', 'absorbed', 'state', 'our', 'bestfit', 'model', 'is', 'consistent', 'with', 'the', 'presence', 'of', 'a', 'l... | [-0.050715798920464294, 0.07979851417515722, 0.02412056071140493, 0.02182884172058645, -0.05380973481320931, -0.19845300959180653, 0.04907917445355755, 0.5110529068527588, -0.14375624317047672, -0.3036311310424935, 0.009744172125768577, -0.3418535086287496, 0.04905653168073817, 0.13690234988583447, 0.030159264539634023... |
710.0383 | Noise and Correlations in a Spatial Population Model with Cyclic
Competition | Noise and spatial degrees of freedom characterize most ecosystems. Some
aspects of their influence on the coevolution of populations with cyclic
interspecies competition have been demonstrated in recent experiments [e.g. B.
Kerr et al., Nature {\bf 418}, 171 (2002)]. To reach a better theoretical
understanding of the... | q-bio.PE cond-mat.stat-mech physics.bio-ph q-bio.QM | noise and spatial degrees of freedom characterize most ecosystems some aspects of their influence on the coevolution of populations with cyclic interspecies competition have been demonstrated in recent experiments eg b kerr et al nature bf 418 171 2002 to reach a better theoretical understanding of these phenomena we c... | [['noise', 'and', 'spatial', 'degrees', 'of', 'freedom', 'characterize', 'most', 'ecosystems', 'some', 'aspects', 'of', 'their', 'influence', 'on', 'the', 'coevolution', 'of', 'populations', 'with', 'cyclic', 'interspecies', 'competition', 'have', 'been', 'demonstrated', 'in', 'recent', 'experiments', 'eg', 'b', 'kerr'... | [-0.12690302251915758, 0.12058053758725389, -0.048533288641677545, 0.08095501907131014, -0.04774650100929042, -0.12096327780745923, -0.0011036080948542803, 0.3509901863678048, -0.24811049416117992, -0.3137770681641996, 0.03809210482577328, -0.2672602166305296, -0.2189882395012925, 0.1502505479787942, 0.0023447576056544... |
710.0384 | The Role of Galactic Winds on Molecular Gas Emission from Galaxy Mergers | We assess the impact of starburst and AGN feedback-driven winds on the CO
emission from galaxy mergers, and, in particular, search for signatures of
these winds in the simulated CO morphologies and emission line profiles. We do
so by combining a 3D non-LTE molecular line radiative transfer code with
smoothed particle... | astro-ph | we assess the impact of starburst and agn feedbackdriven winds on the co emission from galaxy mergers and in particular search for signatures of these winds in the simulated co morphologies and emission line profiles we do so by combining a 3d nonlte molecular line radiative transfer code with smoothed particle hydrody... | [['we', 'assess', 'the', 'impact', 'of', 'starburst', 'and', 'agn', 'feedbackdriven', 'winds', 'on', 'the', 'co', 'emission', 'from', 'galaxy', 'mergers', 'and', 'in', 'particular', 'search', 'for', 'signatures', 'of', 'these', 'winds', 'in', 'the', 'simulated', 'co', 'morphologies', 'and', 'emission', 'line', 'profile... | [-0.059868515417030366, 0.11734462780040804, -0.004124317905945836, 0.1345722375002477, -0.09504306066104591, -0.07345340318527868, -0.014689335740809694, 0.4903864743578691, -0.16700449703812376, -0.3285484877048751, 0.025147961170939304, -0.28764209015984243, 0.04728017666827092, 0.20014546927734372, 0.03098486460856... |
710.0385 | Signatures of LCDM substructure in tidal debris | In the past decade, surveys of the stellar component of the Galaxy have
revealed a number of streams from tidally disrupted dwarf galaxies and globular
clusters. Simulations of hierarchical structure formation in LCDM cosmologies
predict that the dark matter halo of a galaxy like the Milky Way contains
hundreds of su... | astro-ph | in the past decade surveys of the stellar component of the galaxy have revealed a number of streams from tidally disrupted dwarf galaxies and globular clusters simulations of hierarchical structure formation in lcdm cosmologies predict that the dark matter halo of a galaxy like the milky way contains hundreds of subhal... | [['in', 'the', 'past', 'decade', 'surveys', 'of', 'the', 'stellar', 'component', 'of', 'the', 'galaxy', 'have', 'revealed', 'a', 'number', 'of', 'streams', 'from', 'tidally', 'disrupted', 'dwarf', 'galaxies', 'and', 'globular', 'clusters', 'simulations', 'of', 'hierarchical', 'structure', 'formation', 'in', 'lcdm', 'co... | [-0.13989530357134028, 0.08915287806287422, -0.1305718940540986, 0.10910950936258947, -0.10998633584012682, 0.026650485494916422, -0.027320439257470054, 0.3526003102356892, -0.20115561070312085, -0.3711169681839132, 0.02202549640513599, -0.27862502735819283, -0.07016335164645579, 0.20957074101940068, -0.031308711669660... |
710.0386 | Comparing Maintenance Strategies for Overlays | In this paper, we present an analytical tool for understanding the
performance of structured overlay networks under churn based on the
master-equation approach of physics. We motivate and derive an equation for the
average number of hops taken by lookups during churn, for the Chord network. We
analyse this equation i... | cs.NI cond-mat.stat-mech cs.DC | in this paper we present an analytical tool for understanding the performance of structured overlay networks under churn based on the masterequation approach of physics we motivate and derive an equation for the average number of hops taken by lookups during churn for the chord network we analyse this equation in detai... | [['in', 'this', 'paper', 'we', 'present', 'an', 'analytical', 'tool', 'for', 'understanding', 'the', 'performance', 'of', 'structured', 'overlay', 'networks', 'under', 'churn', 'based', 'on', 'the', 'masterequation', 'approach', 'of', 'physics', 'we', 'motivate', 'and', 'derive', 'an', 'equation', 'for', 'the', 'averag... | [-0.11154094742232701, 0.06071925048695448, -0.07575662828821805, 0.06529774682530842, -0.06586896953376709, -0.1372387154460739, 0.10131999462009844, 0.39987954596290365, -0.258229269160438, -0.329513894583215, 0.09359244636016228, -0.2280845016539388, -0.18191315460444457, 0.14996937842261104, -0.08840813928691205, 0... |
710.0387 | Reduced zeta functions of Lie algebras | We define reduced zeta functions of Lie algebras, which can be derived from
motivic zeta functions using the Euler characteristic. We show that reduced
zeta functions of Lie algebras possessing a suitably well-behaved basis are
easy to analyse. We prove that reduced zeta functions are multiplicative under
certain con... | math.RA math.AG | we define reduced zeta functions of lie algebras which can be derived from motivic zeta functions using the euler characteristic we show that reduced zeta functions of lie algebras possessing a suitably wellbehaved basis are easy to analyse we prove that reduced zeta functions are multiplicative under certain condition... | [['we', 'define', 'reduced', 'zeta', 'functions', 'of', 'lie', 'algebras', 'which', 'can', 'be', 'derived', 'from', 'motivic', 'zeta', 'functions', 'using', 'the', 'euler', 'characteristic', 'we', 'show', 'that', 'reduced', 'zeta', 'functions', 'of', 'lie', 'algebras', 'possessing', 'a', 'suitably', 'wellbehaved', 'bas... | [-0.21906435926412715, 0.06412376279155885, -0.18209424486448025, 0.16201855333778878, -0.08532193908066457, -0.14222201378213178, -0.02686987349217565, 0.37322834712164155, -0.3697367997133526, -0.1716105244764737, 0.06941533041315089, -0.12428843525061704, -0.21727074297337695, 0.21898510461223536, -0.054117671599418... |
710.0388 | Hawking radiation from extremal and non-extremal black holes | The relationship between Hawking radiation emitted by non extremal and
extremal Reissner Nordstrom black holes is critically analyzed. A careful study
of a series of regular collapsing geometries reveals that the stress energy
tensor stays regular in the extremal limit and is smoothly connected to that of
non extrema... | hep-th gr-qc | the relationship between hawking radiation emitted by non extremal and extremal reissner nordstrom black holes is critically analyzed a careful study of a series of regular collapsing geometries reveals that the stress energy tensor stays regular in the extremal limit and is smoothly connected to that of non extremal b... | [['the', 'relationship', 'between', 'hawking', 'radiation', 'emitted', 'by', 'non', 'extremal', 'and', 'extremal', 'reissner', 'nordstrom', 'black', 'holes', 'is', 'critically', 'analyzed', 'a', 'careful', 'study', 'of', 'a', 'series', 'of', 'regular', 'collapsing', 'geometries', 'reveals', 'that', 'the', 'stress', 'en... | [-0.1350944319140273, 0.11415519997933561, -0.08841273241187278, 0.15282224370195974, -0.046160183056331364, -0.12764471004174338, 0.006200932313038184, 0.32604427488266136, -0.18117856490928277, -0.2650613677084928, 0.12518491467340387, -0.3349084989536259, -0.13708778450654135, 0.193453135883449, -0.07279036220216709... |
710.0389 | Long wave expansions for water waves over random topography | In this paper, we study the motion of the free surface of a body of fluid
over a variable bottom, in a long wave asymptotic regime. We assume that the
bottom of the fluid region can be described by a stationary random process
$\beta(x, \omega)$ whose variations take place on short length scales and which
are decorrel... | math.AP math-ph math.MP | in this paper we study the motion of the free surface of a body of fluid over a variable bottom in a long wave asymptotic regime we assume that the bottom of the fluid region can be described by a stationary random process betax omega whose variations take place on short length scales and which are decorrelated on the ... | [['in', 'this', 'paper', 'we', 'study', 'the', 'motion', 'of', 'the', 'free', 'surface', 'of', 'a', 'body', 'of', 'fluid', 'over', 'a', 'variable', 'bottom', 'in', 'a', 'long', 'wave', 'asymptotic', 'regime', 'we', 'assume', 'that', 'the', 'bottom', 'of', 'the', 'fluid', 'region', 'can', 'be', 'described', 'by', 'a', '... | [-0.14177403937134406, 0.15359675327947142, -0.10608411338678021, 0.05278243948534009, -0.04498634907835419, -0.07712364968745902, 0.02763153778083717, 0.300061215231519, -0.2887448355710755, -0.23988041056461795, 0.12371373645062018, -0.2615381318011213, -0.16664674155164402, 0.17179740672767418, -0.02905498246969807,... |
710.039 | Moving and ample cones of holomorphic symplectic fourfolds | We analyze the ample and moving cones of holomorphic symplectic manifolds, in
light of recent advances in the minimal model program. As an application, we
establish a numerical criterion for ampleness of divisors on fourfolds
deformation-equivalent to punctual Hilbert schemes of K3 surfaces.
| math.AG | we analyze the ample and moving cones of holomorphic symplectic manifolds in light of recent advances in the minimal model program as an application we establish a numerical criterion for ampleness of divisors on fourfolds deformationequivalent to punctual hilbert schemes of k3 surfaces | [['we', 'analyze', 'the', 'ample', 'and', 'moving', 'cones', 'of', 'holomorphic', 'symplectic', 'manifolds', 'in', 'light', 'of', 'recent', 'advances', 'in', 'the', 'minimal', 'model', 'program', 'as', 'an', 'application', 'we', 'establish', 'a', 'numerical', 'criterion', 'for', 'ampleness', 'of', 'divisors', 'on', 'fo... | [-0.23011136406945976, -0.02538805884589322, -0.11652721293530492, 0.10882339557242948, -0.09002779952661935, -0.186232824084284, 0.029331078424611193, 0.35816574847152416, -0.26904394252355707, -0.20184466201097293, 0.12246671554004383, -0.2532304679585058, -0.17676035911494561, 0.2545039296355965, -0.2299865655341120... |
710.0391 | Dynamical Phase Transitions In Driven Integrate-And-Fire Neurons | We explore the dynamics of an integrate-and-fire neuron with an oscillatory
stimulus. The frustration due to the competition between the neuron's natural
firing period and that of the oscillatory rhythm, leads to a rich structure of
asymptotic phase locking patterns and ordering dynamics. The phase transitions
betwee... | cond-mat.stat-mech cond-mat.dis-nn q-bio.NC | we explore the dynamics of an integrateandfire neuron with an oscillatory stimulus the frustration due to the competition between the neurons natural firing period and that of the oscillatory rhythm leads to a rich structure of asymptotic phase locking patterns and ordering dynamics the phase transitions between these ... | [['we', 'explore', 'the', 'dynamics', 'of', 'an', 'integrateandfire', 'neuron', 'with', 'an', 'oscillatory', 'stimulus', 'the', 'frustration', 'due', 'to', 'the', 'competition', 'between', 'the', 'neurons', 'natural', 'firing', 'period', 'and', 'that', 'of', 'the', 'oscillatory', 'rhythm', 'leads', 'to', 'a', 'rich', '... | [-0.1904907700491651, 0.23181011752321679, -0.10816117031119611, 0.05533448479622983, -0.08706867903451987, -0.16471220408708845, 0.058912982143775314, 0.3529966692345179, -0.344811849752251, -0.23374554684518703, 0.07986791432379003, -0.25737567417019486, -0.2706285046190213, 0.10790391246151483, -0.03416672105216706,... |
710.0392 | Line Broadening in Field Metal-poor Red Giant and Red Horizontal Branch
Stars | We report 349 radial velocities for 45 metal-poor field red giant and red
horizontal branch stars. We have have identified one new spectroscopic binary,
HD 4306, and one possible such system, HD 184711. We also report 57 radial
velocities for 11 of the 91 stars reported on previously by Carney et al.
(2003). As was f... | astro-ph | we report 349 radial velocities for 45 metalpoor field red giant and red horizontal branch stars we have have identified one new spectroscopic binary hd 4306 and one possible such system hd 184711 we also report 57 radial velocities for 11 of the 91 stars reported on previously by carney et al 2003 as was found in the ... | [['we', 'report', '349', 'radial', 'velocities', 'for', '45', 'metalpoor', 'field', 'red', 'giant', 'and', 'red', 'horizontal', 'branch', 'stars', 'we', 'have', 'have', 'identified', 'one', 'new', 'spectroscopic', 'binary', 'hd', '4306', 'and', 'one', 'possible', 'such', 'system', 'hd', '184711', 'we', 'also', 'report'... | [-0.06921703294968941, 0.13439070743600456, -0.021878859343033442, 0.022558062700521936, -0.12172854398573998, -0.05333928996697068, 0.07857467367110485, 0.4423136768246096, -0.081048487939357, -0.4078014187095031, 0.035820905926709494, -0.32096352769901426, -0.07818982684591287, 0.2379921717453124, -0.1043605080906762... |
710.0393 | Quark scattering amplitudes at strong coupling | Following Alday and Maldacena, we describe a string theory method to compute
the strong coupling behavior of the scattering amplitudes of quarks and gluons
in planar N=2 super Yang-Mills theory in the probe approximation. Explicit
predictions for these quantities can be constructed using the all-orders planar
gluon s... | hep-th | following alday and maldacena we describe a string theory method to compute the strong coupling behavior of the scattering amplitudes of quarks and gluons in planar n2 super yangmills theory in the probe approximation explicit predictions for these quantities can be constructed using the allorders planar gluon scatteri... | [['following', 'alday', 'and', 'maldacena', 'we', 'describe', 'a', 'string', 'theory', 'method', 'to', 'compute', 'the', 'strong', 'coupling', 'behavior', 'of', 'the', 'scattering', 'amplitudes', 'of', 'quarks', 'and', 'gluons', 'in', 'planar', 'n2', 'super', 'yangmills', 'theory', 'in', 'the', 'probe', 'approximation'... | [-0.06036443874176781, 0.25522155682477404, -0.16153968846962108, 0.19205040336286616, -0.0369244437759458, -0.10683359667437814, -0.01558847736835606, 0.29034100144596425, -0.13206761154756583, -0.23536221411521152, 0.015133699485085021, -0.29776031617075205, -0.19501088374546902, 0.08637672763759807, -0.0050763592313... |
710.0394 | Higman's PORC conjecture for a family of groups | We prove that the number of groups of order $p^n$ whose Frattini subgroup is
central is for fixed $n$ a PORC (`polynomial on residue classes') function of
$p$. This extends a result of G. Higman.
| math.GR | we prove that the number of groups of order pn whose frattini subgroup is central is for fixed n a porc polynomial on residue classes function of p this extends a result of g higman | [['we', 'prove', 'that', 'the', 'number', 'of', 'groups', 'of', 'order', 'pn', 'whose', 'frattini', 'subgroup', 'is', 'central', 'is', 'for', 'fixed', 'n', 'a', 'porc', 'polynomial', 'on', 'residue', 'classes', 'function', 'of', 'p', 'this', 'extends', 'a', 'result', 'of', 'g', 'higman']] | [-0.2614938119160278, 0.06364675624562162, -0.12636412573712213, 0.008734375787233668, -0.053269415781168, -0.08553109400506531, 0.032336589125251135, 0.2747802036149161, -0.2937428935297898, -0.2803021029835301, 0.028065582857068096, -0.2507010313017028, -0.09430647123205875, 0.20017669993851867, -0.1148916833102703, ... |
710.0395 | Bootes II: Not a Dwarf Galaxy but Possibly Shed by One | This paper has been withdrawn due to a photometric calibration error.
| astro-ph | this paper has been withdrawn due to a photometric calibration error | [['this', 'paper', 'has', 'been', 'withdrawn', 'due', 'to', 'a', 'photometric', 'calibration', 'error']] | [-0.07035269791429694, -0.09069797743789175, -0.1957812620834871, -0.021945465917021713, -0.1751320343464613, -0.08926266664639115, 0.03872974251862615, 0.4193097989667546, -0.2527439138767394, -0.3893624344332652, 0.18061141788282178, -0.28396668894724414, -0.07575928707691756, 0.09942180731079796, -0.4570680446076122... |
710.0396 | Higher-order splitting algorithms for solving the nonlinear
Schr\"odinger equation and their instabilities | Since the kinetic and the potential energy term of the real time nonlinear
Schr\"odinger equation can each be solved exactly, the entire equation can be
solved to any order via splitting algorithms. We verified the fourth-order
convergence of some well known algorithms by solving the Gross-Pitaevskii
equation numeric... | physics.comp-ph physics.atom-ph | since the kinetic and the potential energy term of the real time nonlinear schrodinger equation can each be solved exactly the entire equation can be solved to any order via splitting algorithms we verified the fourthorder convergence of some well known algorithms by solving the grosspitaevskii equation numerically all... | [['since', 'the', 'kinetic', 'and', 'the', 'potential', 'energy', 'term', 'of', 'the', 'real', 'time', 'nonlinear', 'schrodinger', 'equation', 'can', 'each', 'be', 'solved', 'exactly', 'the', 'entire', 'equation', 'can', 'be', 'solved', 'to', 'any', 'order', 'via', 'splitting', 'algorithms', 'we', 'verified', 'the', 'f... | [-0.1620318427967438, 0.13145693811676362, -0.08799222867466835, 0.139031163723203, -0.08287994543185634, -0.12847757219833178, 0.0008099652915159716, 0.30028981881226363, -0.32504237437770317, -0.2770105488054509, 0.11951349965588999, -0.25306237503940604, -0.14934343068365918, 0.17832410609329213, 0.03820157343059452... |
710.0397 | Theory of Pulsar Wind Nebulae | Our understanding of Pulsar Wind Nebulae (PWNe), has greatly improved in the
last years thanks to unprecedented high resolution images taken from the
HUBBLE, CHANDRA and XMM satellites. The discovery of complex but similar inner
features, with the presence of unexpected axisymmetric rings and jets, has
prompted a new... | astro-ph | our understanding of pulsar wind nebulae pwne has greatly improved in the last years thanks to unprecedented high resolution images taken from the hubble chandra and xmm satellites the discovery of complex but similar inner features with the presence of unexpected axisymmetric rings and jets has prompted a new investig... | [['our', 'understanding', 'of', 'pulsar', 'wind', 'nebulae', 'pwne', 'has', 'greatly', 'improved', 'in', 'the', 'last', 'years', 'thanks', 'to', 'unprecedented', 'high', 'resolution', 'images', 'taken', 'from', 'the', 'hubble', 'chandra', 'and', 'xmm', 'satellites', 'the', 'discovery', 'of', 'complex', 'but', 'similar'... | [-0.06645784490906866, 0.07106755347676062, -0.10055872429871843, 0.079630755232992, -0.13694351692265147, -0.07444404349194239, 0.00544123891088126, 0.40596622074141153, -0.23309704931649974, -0.3491205909737834, 0.08135350962741074, -0.266209152063956, -0.0618392143536497, 0.2204961431189317, -0.03854245141335817, -0... |
710.0398 | Spin Supersolid in Anisotropic Spin-One Heisenberg Chain | We consider an S=1 Heisenberg chain with strong exchange (Delta) and
single--ion uniaxial anisotropy (D) in a magnetic field (B) along the symmetry
axis. The low energy spectrum is described by an effective S=1/2 XXZ model that
acts on two different low energy sectors for a given window of fields. The
vacuum of each ... | cond-mat.str-el | we consider an s1 heisenberg chain with strong exchange delta and singleion uniaxial anisotropy d in a magnetic field b along the symmetry axis the low energy spectrum is described by an effective s12 xxz model that acts on two different low energy sectors for a given window of fields the vacuum of each sector exhibits... | [['we', 'consider', 'an', 's1', 'heisenberg', 'chain', 'with', 'strong', 'exchange', 'delta', 'and', 'singleion', 'uniaxial', 'anisotropy', 'd', 'in', 'a', 'magnetic', 'field', 'b', 'along', 'the', 'symmetry', 'axis', 'the', 'low', 'energy', 'spectrum', 'is', 'described', 'by', 'an', 'effective', 's12', 'xxz', 'model',... | [-0.24202255439817064, 0.25356402469693595, -0.03233518833737998, 0.04302449091559365, -0.048142581277837354, -0.1433526687701011, 0.01304968540955867, 0.3918431523122958, -0.25071843935265425, -0.2582118207677489, 0.0410211198076251, -0.29201162638408795, -0.057781974208496865, 0.13874930542938058, 0.12237298804823132... |
710.0399 | Inhomogeneous Diophantine approximation of some Hurwitzian numbers | We continue the work of Takao Komatsu by considering the inhomogeneous
approximation constant L(\theta,\phi) for Hurwitzian numbers \theta, and
rationally related \phi(r \theta +m)/n in Q(\theta) +Q. The current work uses a
compactness theorem to relate such inhomogeneous constants to the homogeneous
approximation co... | math.NT | we continue the work of takao komatsu by considering the inhomogeneous approximation constant lthetaphi for hurwitzian numbers theta and rationally related phir theta mn in qtheta q the current work uses a compactness theorem to relate such inhomogeneous constants to the homogeneous approximation constants among the ne... | [['we', 'continue', 'the', 'work', 'of', 'takao', 'komatsu', 'by', 'considering', 'the', 'inhomogeneous', 'approximation', 'constant', 'lthetaphi', 'for', 'hurwitzian', 'numbers', 'theta', 'and', 'rationally', 'related', 'phir', 'theta', 'mn', 'in', 'qtheta', 'q', 'the', 'current', 'work', 'uses', 'a', 'compactness', '... | [-0.17138690296560527, 0.1442731170582452, -0.0582959044990795, 0.0448903867791939, -0.06325376201421022, -0.11835784545567418, 0.05075847419377948, 0.292109989986888, -0.24683786698483995, -0.27216783958886354, 0.07322966279295673, -0.23789362998504657, -0.1303786937014333, 0.20052361786365508, -0.03053080036437937, 0... |
710.04 | Metal-insulator transition from combined disorder and interaction
effects in Hubbard-like electronic lattice models with random hopping | We uncover a disorder-driven instability in the diffusive Fermi liquid phase
of a class of many-fermion systems, indicative of a metal-insulator transition
of first order type, which arises solely from the competition between quenched
disorder and interparticle interactions. Our result is expected to be relevant
for ... | cond-mat.dis-nn | we uncover a disorderdriven instability in the diffusive fermi liquid phase of a class of manyfermion systems indicative of a metalinsulator transition of first order type which arises solely from the competition between quenched disorder and interparticle interactions our result is expected to be relevant for sufficie... | [['we', 'uncover', 'a', 'disorderdriven', 'instability', 'in', 'the', 'diffusive', 'fermi', 'liquid', 'phase', 'of', 'a', 'class', 'of', 'manyfermion', 'systems', 'indicative', 'of', 'a', 'metalinsulator', 'transition', 'of', 'first', 'order', 'type', 'which', 'arises', 'solely', 'from', 'the', 'competition', 'between'... | [-0.20059056068096062, 0.22493734036069166, -0.03765815881663858, 0.07685362959626432, 0.002695609905726194, -0.19116377645781646, 0.0707415931062903, 0.3140189227346769, -0.2167683403214837, -0.26854055428274853, 0.01672390247018912, -0.30246769961548337, -0.17374982258907573, 0.07701962660426301, 0.04522681865937022,... |
710.0401 | The impact of localized overlap eigenmodes on RMT measurements and
topology | The low energy eigenmodes of the continuum QCD Dirac operator are extended,
but on the lattice, due to discretization effects, the Dirac operator can have
localized eigenmodes. These non-physical modes can introduce strong lattice
artifacts for observables that are sensitive to chiral symmetry, especially in
mixed ac... | hep-lat | the low energy eigenmodes of the continuum qcd dirac operator are extended but on the lattice due to discretization effects the dirac operator can have localized eigenmodes these nonphysical modes can introduce strong lattice artifacts for observables that are sensitive to chiral symmetry especially in mixed action sim... | [['the', 'low', 'energy', 'eigenmodes', 'of', 'the', 'continuum', 'qcd', 'dirac', 'operator', 'are', 'extended', 'but', 'on', 'the', 'lattice', 'due', 'to', 'discretization', 'effects', 'the', 'dirac', 'operator', 'can', 'have', 'localized', 'eigenmodes', 'these', 'nonphysical', 'modes', 'can', 'introduce', 'strong', '... | [-0.1493840928918584, 0.25594785992105146, -0.08352720356962987, 0.09280341150435178, -0.10585660530915975, -0.06503435729169532, 0.030330564440718216, 0.39730351535897507, -0.23347292633996786, -0.22393967554365335, 0.11545460555230659, -0.3350911926184046, -0.14665236552307187, 0.08711130377885543, 0.0051955608283414... |
710.0402 | The XMM-Newton Serendipitous Survey V. Optical identification of the
XMM-Newton Medium sensitivity Survey (XMS) | We present the XMM-Newton Medium sensitivity Survey (XMS), including a total
of 318 X-ray sources found among the serendipitous content of 25 XMM-Newton
target fields. The XMS comprises four largely overlapping source samples
selected at soft (0.5-2 keV), intermediate (0.5-4.5 keV), hard (2-10 keV) and
ultra-hard (4.... | astro-ph | we present the xmmnewton medium sensitivity survey xms including a total of 318 xray sources found among the serendipitous content of 25 xmmnewton target fields the xms comprises four largely overlapping source samples selected at soft 052 kev intermediate 0545 kev hard 210 kev and ultrahard 4575 kev bands the first th... | [['we', 'present', 'the', 'xmmnewton', 'medium', 'sensitivity', 'survey', 'xms', 'including', 'a', 'total', 'of', '318', 'xray', 'sources', 'found', 'among', 'the', 'serendipitous', 'content', 'of', '25', 'xmmnewton', 'target', 'fields', 'the', 'xms', 'comprises', 'four', 'largely', 'overlapping', 'source', 'samples', ... | [-0.041286458045413546, 0.15998050660074858, 0.01067322847772051, 0.11186340279580856, -0.040574620723385704, -0.05785264570096677, 0.1579746293443763, 0.4927935561334545, -0.14780868887477977, -0.4428172600540248, 0.05585850914880707, -0.39584524903700435, 0.06808782005788419, 0.17689498680940066, -0.00165671255354854... |
710.0403 | Area-expanding embeddings of rectangles | We estimate whether there is an embedding from one n-dimensional rectangle
into another which expands every k-dimensional area. Our estimate is sharp up
to a constant factor in each dimension.
| math.DG | we estimate whether there is an embedding from one ndimensional rectangle into another which expands every kdimensional area our estimate is sharp up to a constant factor in each dimension | [['we', 'estimate', 'whether', 'there', 'is', 'an', 'embedding', 'from', 'one', 'ndimensional', 'rectangle', 'into', 'another', 'which', 'expands', 'every', 'kdimensional', 'area', 'our', 'estimate', 'is', 'sharp', 'up', 'to', 'a', 'constant', 'factor', 'in', 'each', 'dimension']] | [-0.05422804607854535, 0.08408329197021279, -0.035934855897600454, -0.011505617224611343, -0.06080997649890681, -0.18716398272663354, 0.037969279816995063, 0.3527883062760035, -0.32119753075142704, -0.1948548913622896, 0.12650934348736578, -0.33231012262403964, -0.12323560800480966, 0.18040776799122493, -0.122233678804... |
710.0404 | Rolling Tachyon in Nonlocal Cosmology | Nonlocal cosmological models derived from String Field Theory are considered.
A new method for constructing rolling tachyon solutions in the FRW metric in
two field configuration is proposed and solutions of the Friedman equations
with nonlocal operator are presented. The cosmological properties of these
solutions ar... | hep-th | nonlocal cosmological models derived from string field theory are considered a new method for constructing rolling tachyon solutions in the frw metric in two field configuration is proposed and solutions of the friedman equations with nonlocal operator are presented the cosmological properties of these solutions are di... | [['nonlocal', 'cosmological', 'models', 'derived', 'from', 'string', 'field', 'theory', 'are', 'considered', 'a', 'new', 'method', 'for', 'constructing', 'rolling', 'tachyon', 'solutions', 'in', 'the', 'frw', 'metric', 'in', 'two', 'field', 'configuration', 'is', 'proposed', 'and', 'solutions', 'of', 'the', 'friedman',... | [-0.15708174603059888, 0.06878289280637623, -0.08908381352716303, 0.11209063078623582, -0.10665809248197586, -0.18865826219676973, -0.1319344609336769, 0.3115980913268125, -0.21317614033382307, -0.258691060475688, 0.08899637229958589, -0.27609304721130334, -0.14630280292414605, 0.1853185292888195, -0.02579660505611212,... |
710.0405 | Open-Loop Woofer-Tweeter Control on the LAO Multi-Conjugate Adaptive
Optics Testbed | Advances in micro deformable mirror (DM) technologies such as MEMs, have
stimulated interest in the characteristics of systems that include a high
stroke mirror in series with a high actuator count mirror. This arrangement is
referred to as a woofer-tweeter system. In certain situations it may be
desirable or necessa... | physics.ins-det | advances in micro deformable mirror dm technologies such as mems have stimulated interest in the characteristics of systems that include a high stroke mirror in series with a high actuator count mirror this arrangement is referred to as a woofertweeter system in certain situations it may be desirable or necessary to op... | [['advances', 'in', 'micro', 'deformable', 'mirror', 'dm', 'technologies', 'such', 'as', 'mems', 'have', 'stimulated', 'interest', 'in', 'the', 'characteristics', 'of', 'systems', 'that', 'include', 'a', 'high', 'stroke', 'mirror', 'in', 'series', 'with', 'a', 'high', 'actuator', 'count', 'mirror', 'this', 'arrangement... | [-0.11063197396218866, 0.09806807423632143, -0.08964153797821883, 0.035032100801286443, -0.01213764484819709, -0.19074278506038544, 0.010409937100801743, 0.4302045644013857, -0.2341099709831099, -0.3704695640271213, 0.12468292259731564, -0.2303481444615085, -0.1176794877095262, 0.2597635396974807, -0.14216411086179467,... |
710.0406 | A Population of Massive and Evolved Galaxies at z$\ga$5 | We report results from a search for massive and evolved galaxies at z>5 in
the GOODS southern field. Combining HST ACS, VLT ISAAC and Spitzer IRAC
photometric data, we develop a color selection technique to identify candidates
for being evolved galaxies at high redshifts. The color selection is primarily
based on loc... | astro-ph | we report results from a search for massive and evolved galaxies at z5 in the goods southern field combining hst acs vlt isaac and spitzer irac photometric data we develop a color selection technique to identify candidates for being evolved galaxies at high redshifts the color selection is primarily based on locating t... | [['we', 'report', 'results', 'from', 'a', 'search', 'for', 'massive', 'and', 'evolved', 'galaxies', 'at', 'z5', 'in', 'the', 'goods', 'southern', 'field', 'combining', 'hst', 'acs', 'vlt', 'isaac', 'and', 'spitzer', 'irac', 'photometric', 'data', 'we', 'develop', 'a', 'color', 'selection', 'technique', 'to', 'identify'... | [-0.00046076376794747286, 0.11227533051286658, -0.044006314571766604, 0.1091079170695476, -0.07243522387861664, -0.04722446277634346, 0.07102672858121467, 0.4796151970154061, -0.03353661077750486, -0.4356563750226351, 0.029930489280471397, -0.3413302035699035, 0.06703494780489447, 0.18804400670764623, -0.02055470445268... |
710.0407 | Instabilities of Spiral Shocks -- II. A quasi-steady State in the
multi-phase inhomogeneous ISM | The ``galactic shocks'' \citep{fujimoto68,roberts69} is investigated using a
full three-dimensional hydrodynamic simulations, taking into account
self-gravity of the ISM, radiative cooling, and star formation followed by
energy feedback from supernovae. This is an essential progress from the
previous numerical models... | astro-ph | the galactic shocks citepfujimoto68roberts69 is investigated using a full threedimensional hydrodynamic simulations taking into account selfgravity of the ism radiative cooling and star formation followed by energy feedback from supernovae this is an essential progress from the previous numerical models in which 2d iso... | [['the', 'galactic', 'shocks', 'citepfujimoto68roberts69', 'is', 'investigated', 'using', 'a', 'full', 'threedimensional', 'hydrodynamic', 'simulations', 'taking', 'into', 'account', 'selfgravity', 'of', 'the', 'ism', 'radiative', 'cooling', 'and', 'star', 'formation', 'followed', 'by', 'energy', 'feedback', 'from', 's... | [-0.12141086045699194, 0.1274782597097801, -0.07964204125665128, 0.10872943645063787, -0.08556321317702532, -0.03287071471661329, -0.03257748156785965, 0.3966580993458629, -0.2705500163063407, -0.25687636001594366, 0.06417652119044215, -0.2245387470573187, -0.07389560903050005, 0.16915483199898154, 0.02188888575497549,... |
710.0408 | Optimal Transportation under Nonholonomic Constraints | We study Monge's optimal transportation problem, where the cost is given by
optimal control cost. We prove the existence and uniqueness of an optimal map
under certain regularity conditions on the Lagrangian, absolute continuity of
the measures with respect to Lebesgue, and most importantly the absence of
sharp abnor... | math.OC math.DG | we study monges optimal transportation problem where the cost is given by optimal control cost we prove the existence and uniqueness of an optimal map under certain regularity conditions on the lagrangian absolute continuity of the measures with respect to lebesgue and most importantly the absence of sharp abnormal min... | [['we', 'study', 'monges', 'optimal', 'transportation', 'problem', 'where', 'the', 'cost', 'is', 'given', 'by', 'optimal', 'control', 'cost', 'we', 'prove', 'the', 'existence', 'and', 'uniqueness', 'of', 'an', 'optimal', 'map', 'under', 'certain', 'regularity', 'conditions', 'on', 'the', 'lagrangian', 'absolute', 'cont... | [-0.1465723511982315, 0.0366101787581451, -0.04326416845791615, 0.10344091035949532, -0.049229232198111, -0.11554678487860096, 0.043538278371740416, 0.3814243310525154, -0.3000083192029986, -0.22891636992314418, 0.15981846803445549, -0.29339803733343545, -0.16873364732600749, 0.17525963299871924, -0.1663713459162794, 0... |
710.0409 | On potentially $K_{r+1}-U$-graphical Sequences | Let $K_{m}-H$ be the graph obtained from $K_{m}$ by removing the edges set
$E(H)$ of the graph $H$ ($H$ is a subgraph of $K_{m}$). We use the symbol $Z_4$
to denote $K_4-P_2.$ A sequence $S$ is potentially $K_{m}-H$-graphical if it
has a realization containing a $K_{m}-H$ as a subgraph. Let $\sigma(K_{m}-H,
n)$ denot... | math.CO | let k_mh be the graph obtained from k_m by removing the edges set eh of the graph h h is a subgraph of k_m we use the symbol z_4 to denote k_4p_2 a sequence s is potentially k_mhgraphical if it has a realization containing a k_mh as a subgraph let sigmak_mh n denote the smallest degree sum such that every nterm graphic... | [['let', 'k_mh', 'be', 'the', 'graph', 'obtained', 'from', 'k_m', 'by', 'removing', 'the', 'edges', 'set', 'eh', 'of', 'the', 'graph', 'h', 'h', 'is', 'a', 'subgraph', 'of', 'k_m', 'we', 'use', 'the', 'symbol', 'z_4', 'to', 'denote', 'k_4p_2', 'a', 'sequence', 's', 'is', 'potentially', 'k_mhgraphical', 'if', 'it', 'has... | [-0.27267154682626465, 0.19701402924831934, 0.04226271394284421, -0.04366173691526997, -0.083288765448313, -0.23779111959071558, 0.03901091210931289, 0.36831862716987895, -0.21848009586376085, -0.27486931446814133, 0.07851458188562309, -0.44621670036838296, -0.0790747135309921, 0.050810874649061914, -0.0859804264808680... |
710.041 | The Theory of Unified Relativity for a Biovielectroluminescence
Phenomenon via Fly's Visual and Imaging System | The elucidation upon fly's neuronal patterns as a link to computer graphics
and memory cards I/O's, is investigated for the phenomenon by propounding a
unified theory of Einstein's two known relativities. It is conclusive that
flies could contribute a certain amount of neuromatrices indicating an imagery
function of ... | cs.CE cs.CV | the elucidation upon flys neuronal patterns as a link to computer graphics and memory cards ios is investigated for the phenomenon by propounding a unified theory of einsteins two known relativities it is conclusive that flies could contribute a certain amount of neuromatrices indicating an imagery function of a visual... | [['the', 'elucidation', 'upon', 'flys', 'neuronal', 'patterns', 'as', 'a', 'link', 'to', 'computer', 'graphics', 'and', 'memory', 'cards', 'ios', 'is', 'investigated', 'for', 'the', 'phenomenon', 'by', 'propounding', 'a', 'unified', 'theory', 'of', 'einsteins', 'two', 'known', 'relativities', 'it', 'is', 'conclusive', ... | [-0.13108423736525765, 0.09691205246798518, -0.06467024467201554, 0.029084961984608526, -0.0778251664032723, -0.2186097668181901, 0.06898934776518217, 0.42645648083271226, -0.2735568679709104, -0.3445249404921924, 0.08682334506784173, -0.28716003967292636, -0.130759166471762, 0.24164824102564353, -0.10897794494758273, ... |
710.0411 | Theoretical topics in spacetime-symmetry violations | The Lorentz- and CPT-violating Chern-Simons extension of electrodynamics is
considered. In the context of N=4 supergravity in four spacetime dimensions, it
is argued that cosmological solutions can generate this extension. Within
Chern-Simons electrodynamics, theoretical and phenomenological topics are
reviewed that ... | hep-th | the lorentz and cptviolating chernsimons extension of electrodynamics is considered in the context of n4 supergravity in four spacetime dimensions it is argued that cosmological solutions can generate this extension within chernsimons electrodynamics theoretical and phenomenological topics are reviewed that concern the... | [['the', 'lorentz', 'and', 'cptviolating', 'chernsimons', 'extension', 'of', 'electrodynamics', 'is', 'considered', 'in', 'the', 'context', 'of', 'n4', 'supergravity', 'in', 'four', 'spacetime', 'dimensions', 'it', 'is', 'argued', 'that', 'cosmological', 'solutions', 'can', 'generate', 'this', 'extension', 'within', 'c... | [-0.1551209126073108, 0.19901196837977128, -0.017021793458196852, 0.12363787920912728, -0.11190261941886058, -0.1474363338202238, -0.10830167053198372, 0.28524384632948097, -0.11375563017403086, -0.29837096027202076, 0.060754039212716396, -0.29873192182707564, -0.17762587697210688, 0.12057119428559586, -0.0557788840658... |
710.0412 | What's up with IR gluon and ghost propagators in Landau gauge? A
puzzling answer from huge lattices | Several analytic approaches predict for SU(N_c) Yang-Mills theories in Landau
gauge an enhanced ghost propagator G(p^2) and a suppressed gluon propagator
D(p^2) at small momenta. This prediction applies to two, three and four
space-time dimensions. Moreover, the gluon propagator is predicted to be null
at p = 0. Nume... | hep-lat | several analytic approaches predict for sun_c yangmills theories in landau gauge an enhanced ghost propagator gp2 and a suppressed gluon propagator dp2 at small momenta this prediction applies to two three and four spacetime dimensions moreover the gluon propagator is predicted to be null at p 0 numerical studies by se... | [['several', 'analytic', 'approaches', 'predict', 'for', 'sun_c', 'yangmills', 'theories', 'in', 'landau', 'gauge', 'an', 'enhanced', 'ghost', 'propagator', 'gp2', 'and', 'a', 'suppressed', 'gluon', 'propagator', 'dp2', 'at', 'small', 'momenta', 'this', 'prediction', 'applies', 'to', 'two', 'three', 'and', 'four', 'spa... | [-0.07903652713611359, 0.198846012175157, -0.1155351708904363, 0.10958340347946122, -0.0320798082200515, -0.13394871919029733, 0.0386955023777285, 0.3776581233776197, -0.14462552599228418, -0.27547318719600034, 0.0756389048484313, -0.3275888414570789, -0.06760844329667345, 0.15850609103217722, 0.031009445288119178, 0.0... |
710.0413 | Chiral behaviour of Delta B = 2 and Delta C =2 matrix elements | We investigate the light-quark mass and spatial volume dependence of matrix
elements of Delta B = 2 and Delta C = 2 four-fermion operators. These operators
are relevant for Neutral B(s) and D mixing in and beyond the Standard Model. An
important conclusion of this work is that the chiral extrapolations for matrix
ele... | hep-lat | we investigate the lightquark mass and spatial volume dependence of matrix elements of delta b 2 and delta c 2 fourfermion operators these operators are relevant for neutral bs and d mixing in and beyond the standard model an important conclusion of this work is that the chiral extrapolations for matrix elements of hea... | [['we', 'investigate', 'the', 'lightquark', 'mass', 'and', 'spatial', 'volume', 'dependence', 'of', 'matrix', 'elements', 'of', 'delta', 'b', '2', 'and', 'delta', 'c', '2', 'fourfermion', 'operators', 'these', 'operators', 'are', 'relevant', 'for', 'neutral', 'bs', 'and', 'd', 'mixing', 'in', 'and', 'beyond', 'the', 's... | [-0.05860069876022559, 0.24068061431353271, 0.03279504363632037, 0.09757821111189616, 0.00910206441120762, -0.1642458885649426, 0.06370307016186416, 0.32803458695869064, -0.22082066177002466, -0.23841418699723566, 0.03680763732376767, -0.3155074846775581, -0.10401481946205927, 0.08457776584934133, 0.0608770690806624, 0... |
710.0414 | Electron as soliton: Nonlinear theory of dielectric polarization | We describe a class of theories of dielectric polarization and a species of
solitons in these theories. The solitons, made entirely out of the polarization
field, have quantized values of the electric charge and can be interpreted as
electrons and holes. A soliton-antisoliton pair is an exciton. We present
numerical ... | cond-mat.mes-hall cond-mat.other | we describe a class of theories of dielectric polarization and a species of solitons in these theories the solitons made entirely out of the polarization field have quantized values of the electric charge and can be interpreted as electrons and holes a solitonantisoliton pair is an exciton we present numerical evidence... | [['we', 'describe', 'a', 'class', 'of', 'theories', 'of', 'dielectric', 'polarization', 'and', 'a', 'species', 'of', 'solitons', 'in', 'these', 'theories', 'the', 'solitons', 'made', 'entirely', 'out', 'of', 'the', 'polarization', 'field', 'have', 'quantized', 'values', 'of', 'the', 'electric', 'charge', 'and', 'can', ... | [-0.20296722688107638, 0.19876367882483337, -0.09105344786586468, 0.07733194059855714, -0.011354188095745548, -0.1126128942542301, 0.006756265578268652, 0.41186058468985975, -0.19908229653772555, -0.24185422033463655, 0.02265461521394747, -0.2688943844353944, -0.11044327858447407, 0.16564920888560122, 0.042445125499446... |
710.0415 | Measurement of triple differential photon plus jet cross section by D0 | We report on a new measurement of triple differential cross section for the
process ppbar -> photon + jet + X in ppbar collisions at sqrt(s)=1.96 TeV by
the D0 Collaboration at Fermilab based on a dataset corresponding to an
integrated luminosity of 1.1 fb-1.
| hep-ex | we report on a new measurement of triple differential cross section for the process ppbar photon jet x in ppbar collisions at sqrts196 tev by the d0 collaboration at fermilab based on a dataset corresponding to an integrated luminosity of 11 fb1 | [['we', 'report', 'on', 'a', 'new', 'measurement', 'of', 'triple', 'differential', 'cross', 'section', 'for', 'the', 'process', 'ppbar', 'photon', 'jet', 'x', 'in', 'ppbar', 'collisions', 'at', 'sqrts196', 'tev', 'by', 'the', 'd0', 'collaboration', 'at', 'fermilab', 'based', 'on', 'a', 'dataset', 'corresponding', 'to',... | [-0.019292112572916915, 0.11108907121490033, -0.10775291733443737, 0.09957726675223794, -0.02147025165946356, -0.0736498978166353, -0.004326306083904845, 0.3818848512711979, -0.12508515940446938, -0.3439559331163764, -0.05169451214827686, -0.4793558356662591, 0.19764359126843156, 0.19139112847014553, 0.0897827176377177... |
710.0416 | Effective Dynamics, Big Bounces and Scaling Symmetry in Bianchi Type I
Loop Quantum Cosmology | The detailed formulation for loop quantum cosmology (LQC) in the Bianchi I
model with a scalar massless field has been constructed. In this paper, its
effective dynamics is studied in two improved strategies for implementing the
LQC discreteness corrections. Both schemes show that the big bang is replaced
by the big ... | gr-qc | the detailed formulation for loop quantum cosmology lqc in the bianchi i model with a scalar massless field has been constructed in this paper its effective dynamics is studied in two improved strategies for implementing the lqc discreteness corrections both schemes show that the big bang is replaced by the big bounces... | [['the', 'detailed', 'formulation', 'for', 'loop', 'quantum', 'cosmology', 'lqc', 'in', 'the', 'bianchi', 'i', 'model', 'with', 'a', 'scalar', 'massless', 'field', 'has', 'been', 'constructed', 'in', 'this', 'paper', 'its', 'effective', 'dynamics', 'is', 'studied', 'in', 'two', 'improved', 'strategies', 'for', 'impleme... | [-0.13890977805254587, 0.17217420716981657, -0.11459234995823918, 0.08107746906550319, -0.03993376149005736, -0.17410960440862586, -0.020881372187145506, 0.3214916764560974, -0.264141694100743, -0.2852385223645604, 0.08699495640907888, -0.22251683310323367, -0.09988410162005687, 0.166959031513243, -0.035932174499965074... |
710.0417 | Quantum capacity of lossy channel with additive classical Gaussian noise
: a perturbation approach | For a quantum channel of additive Gaussian noise with loss, in the general
case of $n$ copies input, we show that up to first order perturbation, any
non-Gaussian perturbation to the product thermal state input has a less quantum
information transmission rate when the input energy tend to infinitive.
| quant-ph | for a quantum channel of additive gaussian noise with loss in the general case of n copies input we show that up to first order perturbation any nongaussian perturbation to the product thermal state input has a less quantum information transmission rate when the input energy tend to infinitive | [['for', 'a', 'quantum', 'channel', 'of', 'additive', 'gaussian', 'noise', 'with', 'loss', 'in', 'the', 'general', 'case', 'of', 'n', 'copies', 'input', 'we', 'show', 'that', 'up', 'to', 'first', 'order', 'perturbation', 'any', 'nongaussian', 'perturbation', 'to', 'the', 'product', 'thermal', 'state', 'input', 'has', '... | [-0.12382248850843432, 0.1476414876001678, -0.07205606327031036, 0.033406450128068726, -0.016613145558429614, -0.16249177086033992, 0.038690752150224786, 0.34744145896057693, -0.30015565266794697, -0.2721134028112402, 0.09070448514444715, -0.29511432471323984, -0.11193177425682697, 0.12510885360023502, -0.0800541699768... |
710.0418 | Neutron Star Crustal Mass Fractions | We are investigating mass fractions on the crust of a neutron star which
would remain after one year of cooling. We use cooling curves corresponding
with various densities, or depths, of the neutron star just after its
formation. We assume the modified Urca process dominates the energy budget of
the outer layers of t... | astro-ph | we are investigating mass fractions on the crust of a neutron star which would remain after one year of cooling we use cooling curves corresponding with various densities or depths of the neutron star just after its formation we assume the modified urca process dominates the energy budget of the outer layers of the sta... | [['we', 'are', 'investigating', 'mass', 'fractions', 'on', 'the', 'crust', 'of', 'a', 'neutron', 'star', 'which', 'would', 'remain', 'after', 'one', 'year', 'of', 'cooling', 'we', 'use', 'cooling', 'curves', 'corresponding', 'with', 'various', 'densities', 'or', 'depths', 'of', 'the', 'neutron', 'star', 'just', 'after'... | [-0.031934824081715836, 0.22545926715146974, -0.08273181014574847, 0.07589343675080867, -0.026016300251097257, -0.019667191551355965, 0.08909363519191614, 0.37316712095795584, -0.2319465186607478, -0.29993584564212583, 0.07910485061764685, -0.279720318230704, 0.04182609840063378, 0.20455085517485336, 0.0211093534378270... |
710.0419 | Gravitational Collapse and Radiation of Grand Unified Theory | The infinite gravitational collapse of any supermassive stars should pass
through an energy scale of the grand unified theory (GUT). After
nucleon-decays, the supermassive star will convert nearly all its mass into
energy, and produce the radiation of GUT. It may probably explain some
ultrahigh energy puzzles in astr... | physics.gen-ph | the infinite gravitational collapse of any supermassive stars should pass through an energy scale of the grand unified theory gut after nucleondecays the supermassive star will convert nearly all its mass into energy and produce the radiation of gut it may probably explain some ultrahigh energy puzzles in astrophysics ... | [['the', 'infinite', 'gravitational', 'collapse', 'of', 'any', 'supermassive', 'stars', 'should', 'pass', 'through', 'an', 'energy', 'scale', 'of', 'the', 'grand', 'unified', 'theory', 'gut', 'after', 'nucleondecays', 'the', 'supermassive', 'star', 'will', 'convert', 'nearly', 'all', 'its', 'mass', 'into', 'energy', 'a... | [-0.06126905348824544, 0.2266743480811581, -0.08368589056966205, 0.23324680705057593, -0.13081924171807865, -0.06380537860871603, 0.008240059425588697, 0.33827748661860824, -0.20675264805969265, -0.3473342356375522, 0.07994339437249841, -0.26880128734434644, -0.001497994469375246, 0.19013148648664355, -0.03961698716351... |
710.042 | Leptonic and semileptonic D and D_s decays at B-factories | Recent measurements of branching fractions, form factors and decay constants
of leptonic and semileptonic decays of D_(s)-mesons acquired at experiments
running at the Upsilon(4S) resonance energy are reviewed.
| hep-ex | recent measurements of branching fractions form factors and decay constants of leptonic and semileptonic decays of d_smesons acquired at experiments running at the upsilon4s resonance energy are reviewed | [['recent', 'measurements', 'of', 'branching', 'fractions', 'form', 'factors', 'and', 'decay', 'constants', 'of', 'leptonic', 'and', 'semileptonic', 'decays', 'of', 'd_smesons', 'acquired', 'at', 'experiments', 'running', 'at', 'the', 'upsilon4s', 'resonance', 'energy', 'are', 'reviewed']] | [-0.07515803096100206, 0.30974735554169724, 0.015875903527355857, 0.04258362583264157, -0.07285634212678781, -0.11442819782705219, 0.10411389012113903, 0.28995302733447814, -0.1753434144926292, -0.23501396379261105, -0.010247627368058872, -0.45095869853954623, 0.08238624953837306, 0.17014845712455334, 0.224121360522177... |
710.0421 | DBI Global Strings | In this note we present global string solutions which are a generalization of
the usual field theory global vortices when the kinetic term is DBI. Such
vortices can result from the spontaneous symmetry breaking in the potential
felt by a D3-brane. In a previous paper (0706.0485), the DBI instanton solution
was constr... | hep-th astro-ph gr-qc hep-ph | in this note we present global string solutions which are a generalization of the usual field theory global vortices when the kinetic term is dbi such vortices can result from the spontaneous symmetry breaking in the potential felt by a d3brane in a previous paper 07060485 the dbi instanton solution was constructed whi... | [['in', 'this', 'note', 'we', 'present', 'global', 'string', 'solutions', 'which', 'are', 'a', 'generalization', 'of', 'the', 'usual', 'field', 'theory', 'global', 'vortices', 'when', 'the', 'kinetic', 'term', 'is', 'dbi', 'such', 'vortices', 'can', 'result', 'from', 'the', 'spontaneous', 'symmetry', 'breaking', 'in', ... | [-0.18792956851339385, 0.11981070479267336, -0.10090334654556338, 0.13138536510228027, -0.08923922563944735, -0.11934769500408378, -0.017033356527707526, 0.2765543632376105, -0.24165859761467176, -0.2478519090531227, 0.08127914095356532, -0.243962541250373, -0.18520758965455775, 0.09716544521441718, -0.0651547104007748... |
710.0422 | Nucleon form factors and structure functions with N_f=2+1 dynamical
domain wall fermions | We report isovector form factors and low moments of structure functions of
nucleon in numerical lattice quantum chromodynamics (QCD) from the on-going
calculations by the RIKEN-BNL-Columbia (RBC) and UKQCD Collaborations with
(2+1) dynamical flavors of domain-wall fermion (DWF) quarks. We calculate the
matrix element... | hep-lat | we report isovector form factors and low moments of structure functions of nucleon in numerical lattice quantum chromodynamics qcd from the ongoing calculations by the rikenbnlcolumbia rbc and ukqcd collaborations with 21 dynamical flavors of domainwall fermion dwf quarks we calculate the matrix elements with four ligh... | [['we', 'report', 'isovector', 'form', 'factors', 'and', 'low', 'moments', 'of', 'structure', 'functions', 'of', 'nucleon', 'in', 'numerical', 'lattice', 'quantum', 'chromodynamics', 'qcd', 'from', 'the', 'ongoing', 'calculations', 'by', 'the', 'rikenbnlcolumbia', 'rbc', 'and', 'ukqcd', 'collaborations', 'with', '21', ... | [-0.10257326067993276, 0.302825825126671, -0.06751601141524699, 0.10198575238764258, -0.04895235091779879, -0.0663989609311102, 0.0850743532249577, 0.3633777515276575, -0.1526013875986929, -0.2919697370221415, -0.0022486824274175997, -0.3166869806661976, -0.01280429464201337, 0.11160813064656616, 0.08163423712054889, 0... |
710.0423 | Effective Lagrangian of Domain Wall Networks | Domain wall networks are studied in N=2 supersymmetric U(N_C) gauge theory
with N_F (>N_C) flavors. We find a systematic method to construct domain wall
networks in terms of moduli matrices. Normalizable moduli parameters of the
network are found to be sizes and phases of the loop. We obtain moduli space
metric which... | hep-th | domain wall networks are studied in n2 supersymmetric un_c gauge theory with n_f n_c flavors we find a systematic method to construct domain wall networks in terms of moduli matrices normalizable moduli parameters of the network are found to be sizes and phases of the loop we obtain moduli space metric which specifies ... | [['domain', 'wall', 'networks', 'are', 'studied', 'in', 'n2', 'supersymmetric', 'un_c', 'gauge', 'theory', 'with', 'n_f', 'n_c', 'flavors', 'we', 'find', 'a', 'systematic', 'method', 'to', 'construct', 'domain', 'wall', 'networks', 'in', 'terms', 'of', 'moduli', 'matrices', 'normalizable', 'moduli', 'parameters', 'of',... | [-0.17111907768373688, 0.1595340253257503, -0.09524219927688439, 0.06906063361248622, -0.07946531628568967, -0.09327722625806928, 0.026004912845479945, 0.4091855963692069, -0.2192753566801548, -0.25456684493149323, 0.09983436801160375, -0.2162711243207256, -0.17880537563314042, 0.07838170600434144, -0.07030173646907012... |
710.0424 | Simulating Magnetohydrodynamical Flow with Constrained Transport and
Adaptive Mesh Refinement; Algorithms & Tests of the AstroBEAR Code | A description is given of the algorithms implemented in the AstroBEAR
adaptive mesh refinement code for ideal magnetohydrodynamics. The code provides
several high resolution, shock capturing schemes which are constructed to
maintain conserved quantities of the flow in a finite volume sense. Divergence
free magnetic f... | astro-ph physics.comp-ph | a description is given of the algorithms implemented in the astrobear adaptive mesh refinement code for ideal magnetohydrodynamics the code provides several high resolution shock capturing schemes which are constructed to maintain conserved quantities of the flow in a finite volume sense divergence free magnetic field ... | [['a', 'description', 'is', 'given', 'of', 'the', 'algorithms', 'implemented', 'in', 'the', 'astrobear', 'adaptive', 'mesh', 'refinement', 'code', 'for', 'ideal', 'magnetohydrodynamics', 'the', 'code', 'provides', 'several', 'high', 'resolution', 'shock', 'capturing', 'schemes', 'which', 'are', 'constructed', 'to', 'ma... | [-0.17227406246478066, 0.0640827184816932, -0.04907846468952758, 0.04202442638736958, -0.04394857954021598, -0.12838788100463502, -0.01893219124587417, 0.3601912868428318, -0.2822933290119502, -0.33928819529383497, 0.13127210436676465, -0.21450313463848195, -0.04523999008404858, 0.21217634478243247, -0.0333323022230829... |
710.0425 | Oscillatory terms in the domain wall transfer matrix | We study the transfer matrix for domain wall fermions to understand the
origin and significance of oscillatory contributions to hadron correlation
functions that arise for M >1. For a free particle in one space, one time, and
one flavor dimension, the eigenmodes of the one-body operator appearing in the
transfer matr... | hep-lat | we study the transfer matrix for domain wall fermions to understand the origin and significance of oscillatory contributions to hadron correlation functions that arise for m 1 for a free particle in one space one time and one flavor dimension the eigenmodes of the onebody operator appearing in the transfer matrix are c... | [['we', 'study', 'the', 'transfer', 'matrix', 'for', 'domain', 'wall', 'fermions', 'to', 'understand', 'the', 'origin', 'and', 'significance', 'of', 'oscillatory', 'contributions', 'to', 'hadron', 'correlation', 'functions', 'that', 'arise', 'for', 'm', '1', 'for', 'a', 'free', 'particle', 'in', 'one', 'space', 'one', ... | [-0.12051010058295526, 0.23208697798957184, -0.05174031159348362, 0.1056381435629465, -0.01572176909861647, -0.12440684244672699, -0.014035568629605392, 0.35609529190128897, -0.21769684877973505, -0.24854397749513146, 0.07763899212733395, -0.3345756077215197, -0.10900267485029451, 0.1484098535881007, 0.0457730305918712... |
710.0426 | Morphologies of Two Massive Old Galaxies at z ~ 2.5 | We present the results of NICMOS imaging of two massive galaxies
photometrically selected to have old stellar populations at z ~ 2.5. Both
galaxies are dominated by apparent disks of old stars, although one of them
also has a small bulge comprising about 1/3 of the light at rest-frame 4800 A.
The presence of massive ... | astro-ph | we present the results of nicmos imaging of two massive galaxies photometrically selected to have old stellar populations at z 25 both galaxies are dominated by apparent disks of old stars although one of them also has a small bulge comprising about 13 of the light at restframe 4800 a the presence of massive disks of o... | [['we', 'present', 'the', 'results', 'of', 'nicmos', 'imaging', 'of', 'two', 'massive', 'galaxies', 'photometrically', 'selected', 'to', 'have', 'old', 'stellar', 'populations', 'at', 'z', '25', 'both', 'galaxies', 'are', 'dominated', 'by', 'apparent', 'disks', 'of', 'old', 'stars', 'although', 'one', 'of', 'them', 'al... | [-0.07350725749334001, 0.16056582363563832, -0.08366024451485525, 0.09079944201382911, -0.04847877939162707, -0.03935031036639379, 0.022135539506389586, 0.39678978850996055, -0.10256460700529041, -0.38099312452875356, 0.06048311152348847, -0.3143673979243936, 0.010278278064948541, 0.1752461802162644, -0.013869886001985... |
710.0427 | Effective Interactions In Neutron-Rich Matter | Properties of effective interactions in neutron-rich matter are reflected in
the medium's equation of state (EOS), which is a relationship among several
state variables. Spin and isospin asymmetries play an important role in the
energy balance and could alter the stability conditions of the nuclear EOS. The
EOS has f... | nucl-th | properties of effective interactions in neutronrich matter are reflected in the mediums equation of state eos which is a relationship among several state variables spin and isospin asymmetries play an important role in the energy balance and could alter the stability conditions of the nuclear eos the eos has farreachin... | [['properties', 'of', 'effective', 'interactions', 'in', 'neutronrich', 'matter', 'are', 'reflected', 'in', 'the', 'mediums', 'equation', 'of', 'state', 'eos', 'which', 'is', 'a', 'relationship', 'among', 'several', 'state', 'variables', 'spin', 'and', 'isospin', 'asymmetries', 'play', 'an', 'important', 'role', 'in', ... | [-0.09553796000804163, 0.20511648574915986, -0.1319891488180942, 0.11976843517199269, -0.09660396073564623, -0.05191496843640891, 0.019071579927347114, 0.30026368560963834, -0.2234034200898818, -0.31806236922123726, 0.0547473483712732, -0.2649225659459036, -0.02561884602675071, 0.18348504074424857, 0.055879090450078626... |
710.0428 | Nature of time and causality in Physics | The conceptual definition and understanding of the nature of time, both
qualitatively and quantitatively is of the utmost difficulty and importance,
and plays a fundamental role in physics. Physical systems seem to evolve in
paths of increasing entropy and of complexity, and thus, the arrow of time
shall be explored ... | gr-qc | the conceptual definition and understanding of the nature of time both qualitatively and quantitatively is of the utmost difficulty and importance and plays a fundamental role in physics physical systems seem to evolve in paths of increasing entropy and of complexity and thus the arrow of time shall be explored in the ... | [['the', 'conceptual', 'definition', 'and', 'understanding', 'of', 'the', 'nature', 'of', 'time', 'both', 'qualitatively', 'and', 'quantitatively', 'is', 'of', 'the', 'utmost', 'difficulty', 'and', 'importance', 'and', 'plays', 'a', 'fundamental', 'role', 'in', 'physics', 'physical', 'systems', 'seem', 'to', 'evolve', ... | [-0.12901088396444851, 0.14718266110867262, -0.11217048375121001, 0.1047906859473317, -0.09058997944313367, -0.1423167394054222, -0.001393161152074234, 0.3181659934239828, -0.2766788139332285, -0.2999823670002765, 0.09052159027591447, -0.217594385418384, -0.13665151630370279, 0.20674592631049954, -0.08910067813745368, ... |
710.0429 | Operated semigroups, Motzkin paths and rooted trees | Combinatorial objects such as rooted trees that carry a recursive structure
have found important applications recently in both mathematics and physics. We
put such structures in an algebraic framework of operated semigroups. This
framework provides the concept of operated semigroups with intuitive and
convenient comb... | math.RA math.CO math.CT | combinatorial objects such as rooted trees that carry a recursive structure have found important applications recently in both mathematics and physics we put such structures in an algebraic framework of operated semigroups this framework provides the concept of operated semigroups with intuitive and convenient combinat... | [['combinatorial', 'objects', 'such', 'as', 'rooted', 'trees', 'that', 'carry', 'a', 'recursive', 'structure', 'have', 'found', 'important', 'applications', 'recently', 'in', 'both', 'mathematics', 'and', 'physics', 'we', 'put', 'such', 'structures', 'in', 'an', 'algebraic', 'framework', 'of', 'operated', 'semigroups',... | [-0.09307029873981507, 0.09642857475584975, -0.1285013660694225, 0.16113448441706457, -0.1647310364708493, -0.11227810089299574, 0.02765620807834158, 0.3472803265705139, -0.33281072935891115, -0.30585588010240206, 0.07329214636171591, -0.22689375203527226, -0.19383775105676318, 0.21745743427743924, -0.1241665794690953,... |
710.043 | Darboux Transformation for the Non-isospectral AKNS Hierarchy and Its
Asymptotic Property | In this article, the Darboux transformation for the non-isospectral AKNS
hierarchy is constructed. We show that the Darboux transformation for the
non-isospectral AKNS hierarchy is not an auto-B\"acklund transformation,
because the integral constants of the hierarchy will be changed after the
transformation. The tran... | math-ph math.MP | in this article the darboux transformation for the nonisospectral akns hierarchy is constructed we show that the darboux transformation for the nonisospectral akns hierarchy is not an autobacklund transformation because the integral constants of the hierarchy will be changed after the transformation the transform rule ... | [['in', 'this', 'article', 'the', 'darboux', 'transformation', 'for', 'the', 'nonisospectral', 'akns', 'hierarchy', 'is', 'constructed', 'we', 'show', 'that', 'the', 'darboux', 'transformation', 'for', 'the', 'nonisospectral', 'akns', 'hierarchy', 'is', 'not', 'an', 'autobacklund', 'transformation', 'because', 'the', '... | [-0.1228126549512025, 0.09449902085846891, -0.08244181583803664, 0.13574778040573518, -0.14659495253322852, -0.12082622746109134, -0.032810209875202015, 0.3165218757155041, -0.425533276465204, -0.22668526580350268, 0.1531152350863623, -0.2478768831739823, -0.22860172535810205, 0.15273294786715674, -0.004844785202294588... |
710.0431 | New Counting Codes for Distributed Video Coding | This paper introduces a new counting code. Its design was motivated by
distributed video coding where, for decoding, error correction methods are
applied to improve predictions. Those error corrections sometimes fail which
results in decoded values worse than the initial prediction. Our code exploits
the fact that bi... | cs.IT math.IT | this paper introduces a new counting code its design was motivated by distributed video coding where for decoding error correction methods are applied to improve predictions those error corrections sometimes fail which results in decoded values worse than the initial prediction our code exploits the fact that bit error... | [['this', 'paper', 'introduces', 'a', 'new', 'counting', 'code', 'its', 'design', 'was', 'motivated', 'by', 'distributed', 'video', 'coding', 'where', 'for', 'decoding', 'error', 'correction', 'methods', 'are', 'applied', 'to', 'improve', 'predictions', 'those', 'error', 'corrections', 'sometimes', 'fail', 'which', 're... | [-0.09185118171472434, 0.07673315658785734, -0.05997036725199621, 0.14818817240654664, -0.01448353528561201, -0.26924508398659763, 0.08001197518700745, 0.3864423849020794, -0.29816651195406346, -0.34335457847993467, 0.10642900489193571, -0.28502960034770664, -0.10183578802296406, 0.22438407803672086, -0.185064897462458... |
710.0432 | Differential Birkhoff decomposition and the renormalization of multiple
zeta values | In the Hopf algebra approach of Connes and Kreimer on renormalization of
quantum field theory, the renormalization process is views as a special case of
the Algebraic Birkhoff Decomposition. We give a differential algebra variation
of this decomposition and apply this to the study of multiple zeta values.
| math.NT math.CO math.RA | in the hopf algebra approach of connes and kreimer on renormalization of quantum field theory the renormalization process is views as a special case of the algebraic birkhoff decomposition we give a differential algebra variation of this decomposition and apply this to the study of multiple zeta values | [['in', 'the', 'hopf', 'algebra', 'approach', 'of', 'connes', 'and', 'kreimer', 'on', 'renormalization', 'of', 'quantum', 'field', 'theory', 'the', 'renormalization', 'process', 'is', 'views', 'as', 'a', 'special', 'case', 'of', 'the', 'algebraic', 'birkhoff', 'decomposition', 'we', 'give', 'a', 'differential', 'algebr... | [-0.18636971101902114, 0.011126181246557584, -0.19706382447232804, 0.07312778050152247, -0.11722793387404333, -0.09986738905233021, 0.020699539534689393, 0.2815858812148993, -0.3603676778730005, -0.20843087519945888, 0.11974997067348643, -0.21616205187456217, -0.19840664932659516, 0.15678201185073704, -0.11726418187996... |
710.0433 | Rota-Baxter operators on generalized power series rings | An important instance of Rota-Baxter algebras from their quantum field theory
application is the ring of Laurent series with a suitable projection. We view
the ring of Laurent series as a special case of generalized power series rings
with exponents in an ordered monoid. We study when a generalized power series
ring ... | math.RA math.CO | an important instance of rotabaxter algebras from their quantum field theory application is the ring of laurent series with a suitable projection we view the ring of laurent series as a special case of generalized power series rings with exponents in an ordered monoid we study when a generalized power series ring has a... | [['an', 'important', 'instance', 'of', 'rotabaxter', 'algebras', 'from', 'their', 'quantum', 'field', 'theory', 'application', 'is', 'the', 'ring', 'of', 'laurent', 'series', 'with', 'a', 'suitable', 'projection', 'we', 'view', 'the', 'ring', 'of', 'laurent', 'series', 'as', 'a', 'special', 'case', 'of', 'generalized',... | [-0.18149259360865333, 0.05184305800671259, -0.10646461454721598, 0.019075266481377185, -0.11057622305189188, -0.11827874215176472, -0.0920765101390246, 0.32648823037206265, -0.43121238118753985, -0.1240315022949989, 0.1259469716505219, -0.25818317229859533, -0.19152291749532407, 0.2048003445737637, -0.1060983873187349... |
710.0434 | I=2 Two-Pion Wave Functions with Non-zero Total Momentum | We calculate the two-pion wave function for the I=2 $S$-wave two-pion system
with a finite scattering momentum and estimate the interaction range between
two pions. It allows us to examine the validity of the necessary condition for
the finite-volume method for the scattering phase shift. A calculation is
carried out... | hep-lat | we calculate the twopion wave function for the i2 swave twopion system with a finite scattering momentum and estimate the interaction range between two pions it allows us to examine the validity of the necessary condition for the finitevolume method for the scattering phase shift a calculation is carried out with a pla... | [['we', 'calculate', 'the', 'twopion', 'wave', 'function', 'for', 'the', 'i2', 'swave', 'twopion', 'system', 'with', 'a', 'finite', 'scattering', 'momentum', 'and', 'estimate', 'the', 'interaction', 'range', 'between', 'two', 'pions', 'it', 'allows', 'us', 'to', 'examine', 'the', 'validity', 'of', 'the', 'necessary', '... | [-0.11678005065783419, 0.22577292641034777, -0.10644772917795811, 0.11518838034902254, -0.011288867053656799, -0.07573368533092163, 0.05843002388473623, 0.36737785716859267, -0.1763004820406298, -0.256194539664614, 0.017506518303590207, -0.30962940376775805, -0.01655162377348054, 0.16233991596685804, 0.0845339368748253... |
710.0435 | Entanglement, recoherence and information flow in an accelerated
detector - quantum field system: Implications for black hole information
issue | We study an exactly solvable model where an uniformly accelerated detector is
linearly coupled to a massless scalar field initially in the Minkowski vacuum.
Using the exact correlation functions we show that as soon as the coupling is
switched on one can see information flowing from the detector to the field and
prop... | gr-qc | we study an exactly solvable model where an uniformly accelerated detector is linearly coupled to a massless scalar field initially in the minkowski vacuum using the exact correlation functions we show that as soon as the coupling is switched on one can see information flowing from the detector to the field and propaga... | [['we', 'study', 'an', 'exactly', 'solvable', 'model', 'where', 'an', 'uniformly', 'accelerated', 'detector', 'is', 'linearly', 'coupled', 'to', 'a', 'massless', 'scalar', 'field', 'initially', 'in', 'the', 'minkowski', 'vacuum', 'using', 'the', 'exact', 'correlation', 'functions', 'we', 'show', 'that', 'as', 'soon', '... | [-0.13126271181298713, 0.16353647508308516, -0.1040485543707906, 0.06149961109233545, -0.0031079516419952337, -0.1388852708456427, -0.006714288367765394, 0.3174469175235734, -0.23772791284749187, -0.28437893761902566, 0.09643504149676395, -0.2981675008296786, -0.09368331080702273, 0.16069940078121267, -0.01850656686380... |
710.0436 | Application of Quantum Theory to Super-parametric Density Estimation | In this paper, we will discuss how to generalize nonparametric density
estimators to MLE parametric estimators. Basing on the Parzen window theory and
using the advantages of probability amplitude of quantum theory, we model a
nonlinear optimization problem and it is very difficult, if not impossible, to
solve the pr... | math.ST stat.TH | in this paper we will discuss how to generalize nonparametric density estimators to mle parametric estimators basing on the parzen window theory and using the advantages of probability amplitude of quantum theory we model a nonlinear optimization problem and it is very difficult if not impossible to solve the problem a... | [['in', 'this', 'paper', 'we', 'will', 'discuss', 'how', 'to', 'generalize', 'nonparametric', 'density', 'estimators', 'to', 'mle', 'parametric', 'estimators', 'basing', 'on', 'the', 'parzen', 'window', 'theory', 'and', 'using', 'the', 'advantages', 'of', 'probability', 'amplitude', 'of', 'quantum', 'theory', 'we', 'mo... | [-0.030296657500104386, 0.022185449158075635, -0.140631121968299, 0.1070755117972168, -0.11141120601840858, -0.16011171485427456, 0.046323761167056735, 0.3557595924874924, -0.27718211138912335, -0.31049530811129167, 0.1331561729142848, -0.2255620338392116, -0.2235603558784741, 0.22904492490118442, -0.1256208610953438, ... |
710.0437 | Connectivity of the Product Replacement Graph of Simple Groups of
Bounded Lie Rank | The Product Replacement Algorithm is a practical algorithm for generating
random elements of a finite group. The algorithm can be described as a random
walk on a graph whose vertices are the generating k-tuples of the group (for a
fixed integer k).
We show that there is a function c(r) such that for any finite simp... | math.GR | the product replacement algorithm is a practical algorithm for generating random elements of a finite group the algorithm can be described as a random walk on a graph whose vertices are the generating ktuples of the group for a fixed integer k we show that there is a function cr such that for any finite simple group of... | [['the', 'product', 'replacement', 'algorithm', 'is', 'a', 'practical', 'algorithm', 'for', 'generating', 'random', 'elements', 'of', 'a', 'finite', 'group', 'the', 'algorithm', 'can', 'be', 'described', 'as', 'a', 'random', 'walk', 'on', 'a', 'graph', 'whose', 'vertices', 'are', 'the', 'generating', 'ktuples', 'of', '... | [-0.17423924765328772, 0.1321266959757381, -0.09607732514898802, 0.014675248633906936, -0.12689020474844603, -0.1450229269193159, 0.0634186445728194, 0.40190407714912113, -0.2556967945942252, -0.23446167845125357, 0.10004310695377668, -0.25595151248711134, -0.1591226239160625, 0.204371549198692, -0.07286650600564695, -... |
710.0438 | A Lattice Formulation of Two Dimensional Topological Field Theory | We propose a non-perturbative criterion to investigate whether supersymmetric
lattice gauge theories preserving partial SUSY can have the desired continuum
limit or not. Since the target continuum theories of the lattice models are
extended supersymmetric gauge theories including the topological field theory
(TFT) as... | hep-lat | we propose a nonperturbative criterion to investigate whether supersymmetric lattice gauge theories preserving partial susy can have the desired continuum limit or not since the target continuum theories of the lattice models are extended supersymmetric gauge theories including the topological field theory tft as a spe... | [['we', 'propose', 'a', 'nonperturbative', 'criterion', 'to', 'investigate', 'whether', 'supersymmetric', 'lattice', 'gauge', 'theories', 'preserving', 'partial', 'susy', 'can', 'have', 'the', 'desired', 'continuum', 'limit', 'or', 'not', 'since', 'the', 'target', 'continuum', 'theories', 'of', 'the', 'lattice', 'model... | [-0.1000781507535987, 0.14153227600395496, -0.11989422415291177, 0.12054007806108091, -0.07490011505828595, -0.15236662007454368, 0.04041196140575648, 0.3657005616337245, -0.2611512784834629, -0.2362723451073247, 0.09548405582159987, -0.21406009326039319, -0.14456035247214324, 0.07395715943255957, -0.08448523214592794,... |
710.0439 | Superconducting properties of Pr-based Filled skutterudite
PrRu$_4$As$_{12}$ | We report on systematic study of superconducting characteristics and Pr
crystalline-electric-field (CEF) levels of filled-skutterudite \pra ($T_{\rm
c}$ = 2.33 K). The temperature dependences of the upper critical field $H_{\rm
c2}$ and the Ginzburg-Landau (Maki) parameter $\kappa_2$ suggest an s-wave
clean-limit sup... | cond-mat.str-el cond-mat.supr-con | we report on systematic study of superconducting characteristics and pr crystallineelectricfield cef levels of filledskutterudite pra t_rm c 233 k the temperature dependences of the upper critical field h_rm c2 and the ginzburglandau maki parameter kappa_2 suggest an swave cleanlimit superconductivity the electronic sp... | [['we', 'report', 'on', 'systematic', 'study', 'of', 'superconducting', 'characteristics', 'and', 'pr', 'crystallineelectricfield', 'cef', 'levels', 'of', 'filledskutterudite', 'pra', 't_rm', 'c', '233', 'k', 'the', 'temperature', 'dependences', 'of', 'the', 'upper', 'critical', 'field', 'h_rm', 'c2', 'and', 'the', 'gi... | [-0.19629012273552898, 0.24826663288023645, 0.04054801268861271, 0.05762457765656738, -0.018238121770823804, -0.1418419432324859, 0.17180911673662755, 0.3288699817413894, -0.1794051337808084, -0.3306114630128902, -0.09544765972980084, -0.3746972883764941, 0.004119381394523841, 0.16035481207968239, 0.1256840504777546, -... |
710.044 | The prospects for constraining dark energy with future X-ray cluster gas
mass fraction measurements | We examine the ability of a future X-ray observatory to constrain dark energy
via measurements of the cluster X-ray gas mass fraction, fgas. We find that
fgas measurements for a sample of ~500 hot, X-ray bright, dynamically relaxed
clusters, to a precision of ~5 per cent, can be used to constrain dark energy
with a D... | astro-ph | we examine the ability of a future xray observatory to constrain dark energy via measurements of the cluster xray gas mass fraction fgas we find that fgas measurements for a sample of 500 hot xray bright dynamically relaxed clusters to a precision of 5 per cent can be used to constrain dark energy with a dark energy ta... | [['we', 'examine', 'the', 'ability', 'of', 'a', 'future', 'xray', 'observatory', 'to', 'constrain', 'dark', 'energy', 'via', 'measurements', 'of', 'the', 'cluster', 'xray', 'gas', 'mass', 'fraction', 'fgas', 'we', 'find', 'that', 'fgas', 'measurements', 'for', 'a', 'sample', 'of', '500', 'hot', 'xray', 'bright', 'dynam... | [-0.05863945312555355, 0.1555857782719024, -0.08949455205337997, 0.1313895133199354, -0.11361854773303362, -0.059031132764829006, 0.09173645389235159, 0.3939621812208149, -0.20241959873934498, -0.43187949367024947, 0.06444288452375602, -0.3178280959935518, 0.013776100919463895, 0.2439633103305285, 0.0304926094593893, 0... |
710.0441 | Comparative Analysis of Non-thermal Emissions and Study of Electron
Transport in a Solar Flare | We study the non-thermal emissions in a solar flare occurring on 2003 May 29
by using RHESSI hard X-ray (HXR) and Nobeyama microwave observations. This
flare shows several typical behaviors of the HXR and microwave emissions: time
delay of microwave peaks relative to HXR peaks, loop-top microwave and
footpoint HXR so... | astro-ph | we study the nonthermal emissions in a solar flare occurring on 2003 may 29 by using rhessi hard xray hxr and nobeyama microwave observations this flare shows several typical behaviors of the hxr and microwave emissions time delay of microwave peaks relative to hxr peaks looptop microwave and footpoint hxr sources and ... | [['we', 'study', 'the', 'nonthermal', 'emissions', 'in', 'a', 'solar', 'flare', 'occurring', 'on', '2003', 'may', '29', 'by', 'using', 'rhessi', 'hard', 'xray', 'hxr', 'and', 'nobeyama', 'microwave', 'observations', 'this', 'flare', 'shows', 'several', 'typical', 'behaviors', 'of', 'the', 'hxr', 'and', 'microwave', 'em... | [-0.07262867890759227, 0.22110012002577634, -0.036674402440542875, 0.17619771397847817, -0.03244177418636139, -0.09212419197933037, 0.0037015460818026636, 0.48998590497319233, -0.2284558519490601, -0.3791851132877709, 0.0033559093813498304, -0.3315531607121997, -0.01367462800873309, 0.24620218381055237, 0.0233991575360... |
710.0442 | Overlapping self-affine sets of Kakeya type | We compute the Minkowski dimension for a family of self-affine sets on the
plane. Our result holds for every (rather than generic) set in the class.
Moreover, we exhibit explicit open subsets of this class where we allow
overlapping, and do not impose any conditions on the norms of the linear maps.
The family under c... | math.CA math.DS | we compute the minkowski dimension for a family of selfaffine sets on the plane our result holds for every rather than generic set in the class moreover we exhibit explicit open subsets of this class where we allow overlapping and do not impose any conditions on the norms of the linear maps the family under considerati... | [['we', 'compute', 'the', 'minkowski', 'dimension', 'for', 'a', 'family', 'of', 'selfaffine', 'sets', 'on', 'the', 'plane', 'our', 'result', 'holds', 'for', 'every', 'rather', 'than', 'generic', 'set', 'in', 'the', 'class', 'moreover', 'we', 'exhibit', 'explicit', 'open', 'subsets', 'of', 'this', 'class', 'where', 'we'... | [-0.12744173793907976, 0.08648620224266779, -0.05548732736497186, 0.07241190774038841, -0.05181154545789468, -0.07264428018970648, 0.042948388238073676, 0.3374408939416753, -0.23916334268869832, -0.2133450475957943, 0.11536657957003627, -0.2611738534938013, -0.14222721036639996, 0.25858941495425825, -0.0866218635492259... |
710.0443 | Tongue-placed tactile biofeedback suppresses the deleterious effects of
muscle fatigue on joint position sense at the ankle | Whereas the acuity of the position sense at the ankle can be disturbed by
muscle fatigue, it recently also has been shown to be improved, under normal
ankle neuromuscular state, through the use of an artificial tongue-placed
tactile biofeedback. The underlying principle of this biofeedback consisted of
supplying indi... | physics.med-ph q-bio.NC | whereas the acuity of the position sense at the ankle can be disturbed by muscle fatigue it recently also has been shown to be improved under normal ankle neuromuscular state through the use of an artificial tongueplaced tactile biofeedback the underlying principle of this biofeedback consisted of supplying individuals... | [['whereas', 'the', 'acuity', 'of', 'the', 'position', 'sense', 'at', 'the', 'ankle', 'can', 'be', 'disturbed', 'by', 'muscle', 'fatigue', 'it', 'recently', 'also', 'has', 'been', 'shown', 'to', 'be', 'improved', 'under', 'normal', 'ankle', 'neuromuscular', 'state', 'through', 'the', 'use', 'of', 'an', 'artificial', 't... | [-0.05378201246305646, 0.12739890334859746, -0.08079156831645214, 0.008463549112306495, -0.0938712865311384, -0.13410412944404426, 0.05521968387482638, 0.4082401745390516, -0.23111552758108792, -0.34567602741404074, 0.0785372292671168, -0.2437273742723371, -0.16404544844015226, 0.1629978873544616, -0.21100844307865546,... |
710.0444 | A note on the two-neutrino decay mode of excited nuclear states | The possibility for the excited nuclear states to decay by emission of the
neutrino-antineutrino pair in direct competition with electromagnetic decay
modes is commented upon.
| nucl-ex | the possibility for the excited nuclear states to decay by emission of the neutrinoantineutrino pair in direct competition with electromagnetic decay modes is commented upon | [['the', 'possibility', 'for', 'the', 'excited', 'nuclear', 'states', 'to', 'decay', 'by', 'emission', 'of', 'the', 'neutrinoantineutrino', 'pair', 'in', 'direct', 'competition', 'with', 'electromagnetic', 'decay', 'modes', 'is', 'commented', 'upon']] | [-0.08030213110148907, 0.33563715681433676, -0.013171140030026436, 0.09775097528938204, -0.05477858171798289, -0.06292688213288784, 0.07814267843961716, 0.34314136803150175, -0.23580916732549667, -0.2380167469382286, -0.04596510397735983, -0.3367943173646927, 0.019888011179864405, 0.14550608932971953, 0.179736477658152... |
710.0445 | Evolution of the genetic code from the GC- to the AGUC-alphabet | A hypothesis of the evolution of the genetic code is proposed, the leading
mechanism of which is the nucleotide spontaneous damage leading to
AT-enrichment of the genome. The hypothesis accounts for stability of the
genetic code towards point mutations, the presence of code dialects, and the
symmetry of the genetic c... | q-bio.PE q-bio.BM | a hypothesis of the evolution of the genetic code is proposed the leading mechanism of which is the nucleotide spontaneous damage leading to atenrichment of the genome the hypothesis accounts for stability of the genetic code towards point mutations the presence of code dialects and the symmetry of the genetic code tab... | [['a', 'hypothesis', 'of', 'the', 'evolution', 'of', 'the', 'genetic', 'code', 'is', 'proposed', 'the', 'leading', 'mechanism', 'of', 'which', 'is', 'the', 'nucleotide', 'spontaneous', 'damage', 'leading', 'to', 'atenrichment', 'of', 'the', 'genome', 'the', 'hypothesis', 'accounts', 'for', 'stability', 'of', 'the', 'ge... | [-0.14409729465842247, 0.06198150045775737, -0.053975653691360585, 0.1164350335781749, 2.258990962917988e-05, -0.13065523798398387, 0.096782345790416, 0.28908437862992287, -0.30298234780247396, -0.262801781995222, 0.07039032220983735, -0.2198792312365885, -0.1661408536422711, 0.11988692325898088, -0.0166492936404071, 0... |
710.0446 | The Detector DCR | The Detector Concept Report (DCR) consists of two parts, one for the physics
and the other for ILC detectors. It has been prepared as the accompany document
of the ILC Accelerator Reference Design Report. The detector DCR describes ILC
detector designs, R&Ds on detector technologies and expected performances. The
ove... | physics.ins-det | the detector concept report dcr consists of two parts one for the physics and the other for ilc detectors it has been prepared as the accompany document of the ilc accelerator reference design report the detector dcr describes ilc detector designs rds on detector technologies and expected performances the overview of t... | [['the', 'detector', 'concept', 'report', 'dcr', 'consists', 'of', 'two', 'parts', 'one', 'for', 'the', 'physics', 'and', 'the', 'other', 'for', 'ilc', 'detectors', 'it', 'has', 'been', 'prepared', 'as', 'the', 'accompany', 'document', 'of', 'the', 'ilc', 'accelerator', 'reference', 'design', 'report', 'the', 'detector... | [-0.0717620805112852, 0.09729519328250298, -0.0309544817529737, 0.00995278627877789, -0.0313392820812407, -0.15451928171964865, -0.08609976118341797, 0.3560458715591166, -0.1830357558256577, -0.3716271494825681, 0.11912280678867347, -0.3859811086385023, -0.05034106978703113, 0.2520153804068705, 0.00694525491682783, 0.1... |
710.0447 | Permutation statistics related to a class of noncommutative symmetric
functions and generalizations of the Genocchi numbers | We prove conjectures of the third author [L. Tevlin, Proc. FPSAC'07, Tianjin]
on two new bases of noncommutative symmetric functions: the transition matrices
from the ribbon basis have nonnegative integral coefficients. This is done by
means of two composition-valued statistics on permutations and packed words,
which... | math.CO | we prove conjectures of the third author l tevlin proc fpsac07 tianjin on two new bases of noncommutative symmetric functions the transition matrices from the ribbon basis have nonnegative integral coefficients this is done by means of two compositionvalued statistics on permutations and packed words which generalize t... | [['we', 'prove', 'conjectures', 'of', 'the', 'third', 'author', 'l', 'tevlin', 'proc', 'fpsac07', 'tianjin', 'on', 'two', 'new', 'bases', 'of', 'noncommutative', 'symmetric', 'functions', 'the', 'transition', 'matrices', 'from', 'the', 'ribbon', 'basis', 'have', 'nonnegative', 'integral', 'coefficients', 'this', 'is', ... | [-0.1742939928158101, 0.13655061833560467, -0.06211011951827273, 0.06888199046406211, -0.09185538325002607, -0.11337764728434231, 0.01927166546656921, 0.29349044254239726, -0.3089452806328024, -0.24575892429114604, 0.08177887215944273, -0.2807673511608523, -0.17579531055704065, 0.17859845810061398, -0.07993454562158, 0... |
710.0448 | Differential Complexes and Stratified Pro-Modules | In this paper we introduce the category of stratified Pro-modules and the
notion of induced object in this category. We propose a translation of a
Morihiko Saito equivalence result using the dual language of Pro-objects. So we
prove an equivalence between the derived category of stratified Pro-modules and
the categor... | math.AG | in this paper we introduce the category of stratified promodules and the notion of induced object in this category we propose a translation of a morihiko saito equivalence result using the dual language of proobjects so we prove an equivalence between the derived category of stratified promodules and the category of pr... | [['in', 'this', 'paper', 'we', 'introduce', 'the', 'category', 'of', 'stratified', 'promodules', 'and', 'the', 'notion', 'of', 'induced', 'object', 'in', 'this', 'category', 'we', 'propose', 'a', 'translation', 'of', 'a', 'morihiko', 'saito', 'equivalence', 'result', 'using', 'the', 'dual', 'language', 'of', 'proobject... | [-0.12499624461810471, 0.05882504522631996, -0.0861166466634269, 0.06469296282474798, -0.0558019746941599, -0.04849455452693457, 0.05066574765827902, 0.3687000004071954, -0.38477567464790563, -0.25817049686994514, 0.013138201616873795, -0.16281045939434657, -0.14931612371495276, 0.12478379690737436, -0.2103892426627377... |
710.0449 | Gravitino dark matter from increased thermal relic particles | We investigate the so-called superWIMP scenario with gravitino as the
lightest supersymmetric particle (LSP) in the context of non-standard
cosmology, in particular, brane world cosmology. As a candidate of the
next-to-LSP (NLSP), we examine slepton and sneutrino. Brane world cosmological
effects dramatically enhance... | hep-ph astro-ph | we investigate the socalled superwimp scenario with gravitino as the lightest supersymmetric particle lsp in the context of nonstandard cosmology in particular brane world cosmology as a candidate of the nexttolsp nlsp we examine slepton and sneutrino brane world cosmological effects dramatically enhance the relic dens... | [['we', 'investigate', 'the', 'socalled', 'superwimp', 'scenario', 'with', 'gravitino', 'as', 'the', 'lightest', 'supersymmetric', 'particle', 'lsp', 'in', 'the', 'context', 'of', 'nonstandard', 'cosmology', 'in', 'particular', 'brane', 'world', 'cosmology', 'as', 'a', 'candidate', 'of', 'the', 'nexttolsp', 'nlsp', 'we... | [-0.08976722220427587, 0.3126837406406677, -0.02870678355578672, 0.24881351083613834, -0.10504991092867302, -0.2110652101026582, -0.02003134033406855, 0.28014758031047254, -0.21946390138261698, -0.36290640197089546, 0.060886971431772234, -0.26627533764853567, 0.07663900654781126, 0.13941809588471765, -0.003084277532323... |
710.045 | Geometric phases in open tripod systems | We first consider stimulated Raman adibatic passages (STIRAP) in a closed
four-level tripod system. In this case, the adiabatic eigenstates of the system
acquire real geometric phases. When the system is open and subject to
decoherence they acquire complex geometric phases that we determine by a Monte
Carlo wave func... | quant-ph | we first consider stimulated raman adibatic passages stirap in a closed fourlevel tripod system in this case the adiabatic eigenstates of the system acquire real geometric phases when the system is open and subject to decoherence they acquire complex geometric phases that we determine by a monte carlo wave function app... | [['we', 'first', 'consider', 'stimulated', 'raman', 'adibatic', 'passages', 'stirap', 'in', 'a', 'closed', 'fourlevel', 'tripod', 'system', 'in', 'this', 'case', 'the', 'adiabatic', 'eigenstates', 'of', 'the', 'system', 'acquire', 'real', 'geometric', 'phases', 'when', 'the', 'system', 'is', 'open', 'and', 'subject', '... | [-0.18821942151213686, 0.1660923797221282, -0.08073034738772548, 0.049028615579785155, 0.05165670229665314, -0.14232254054707785, 0.07169865460600704, 0.36562601577801007, -0.2984182304275843, -0.2836086853562544, 0.09213880635215901, -0.23208830700799202, -0.1598185007237286, 0.20117521546781064, -0.059931452052357295... |
710.0451 | Low temperature magnetization of the S=1/2 kagome antiferromagnet
ZnCu_3(OH)_6Cl_2 | The dc-magnetization of the unique S=1/2 kagome antiferromagnet
Herbertsmithite has been measured down to 0.1K. No sign of spin freezing is
observed in agreement with former muSR and ac-susceptibility results. The low
temperature magnetic response is dominated by a defect contribution which
exhibits a new energy scal... | cond-mat.str-el | the dcmagnetization of the unique s12 kagome antiferromagnet herbertsmithite has been measured down to 01k no sign of spin freezing is observed in agreement with former musr and acsusceptibility results the low temperature magnetic response is dominated by a defect contribution which exhibits a new energy scale simeq 1... | [['the', 'dcmagnetization', 'of', 'the', 'unique', 's12', 'kagome', 'antiferromagnet', 'herbertsmithite', 'has', 'been', 'measured', 'down', 'to', '01k', 'no', 'sign', 'of', 'spin', 'freezing', 'is', 'observed', 'in', 'agreement', 'with', 'former', 'musr', 'and', 'acsusceptibility', 'results', 'the', 'low', 'temperatur... | [-0.16073061194928254, 0.2424989755938227, -0.03968308059608235, 0.028894145675140488, -0.07609187488389366, -0.15662231280139702, 0.06783788090243059, 0.35196545826380743, -0.2144488976939636, -0.30527277402579783, 0.07205368001356392, -0.3549717342590584, -0.02458237752332078, 0.1964748087873244, 0.09704019613564015,... |
710.0452 | Low energy properties of the SU(m|n) supersymmetric Haldane-Shastry spin
chain | The ground state and low energy excitations of the SU(m|n) supersymmetric
Haldane-Shastry spin chain are analyzed. In the thermodynamic limit, it is
found that the ground state degeneracy is finite only for the SU(m|0) and
SU(m|1) spin chains, while the dispersion relation for the low energy and low
momentum excitati... | hep-th cond-mat.stat-mech nlin.SI | the ground state and low energy excitations of the sumn supersymmetric haldaneshastry spin chain are analyzed in the thermodynamic limit it is found that the ground state degeneracy is finite only for the sum0 and sum1 spin chains while the dispersion relation for the low energy and low momentum excitations is linear f... | [['the', 'ground', 'state', 'and', 'low', 'energy', 'excitations', 'of', 'the', 'sumn', 'supersymmetric', 'haldaneshastry', 'spin', 'chain', 'are', 'analyzed', 'in', 'the', 'thermodynamic', 'limit', 'it', 'is', 'found', 'that', 'the', 'ground', 'state', 'degeneracy', 'is', 'finite', 'only', 'for', 'the', 'sum0', 'and',... | [-0.17224708522886806, 0.26846156524003745, -0.01295894406575826, 0.10534281031146844, 0.021603900613974183, -0.15339816373040657, 0.007178671002203158, 0.32961238828267303, -0.21754729569683434, -0.267285727654079, 0.06288143139215228, -0.3239852865973047, -0.038053275907113576, 0.1366411871276796, 0.07693906708350334... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.