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 |
|---|---|---|---|---|---|---|
710.3353 | Roadmap for ILC Detector R&D Test Beams | This document provides a roadmap for ILC detector test beam needs in the next
3 - 5 years. In this period, detector Letters of Intent are expected by fall
2008, the ILC Engineering Design Report to be submitted in ILC and its
detectors in 2012. ILC detectors are required to have unprecedented precision
to be able to ... | physics.ins-det | this document provides a roadmap for ilc detector test beam needs in the next 3 5 years in this period detector letters of intent are expected by fall 2008 the ilc engineering design report to be submitted in ilc and its detectors in 2012 ilc detectors are required to have unprecedented precision to be able to elucidat... | [['this', 'document', 'provides', 'a', 'roadmap', 'for', 'ilc', 'detector', 'test', 'beam', 'needs', 'in', 'the', 'next', '3', '5', 'years', 'in', 'this', 'period', 'detector', 'letters', 'of', 'intent', 'are', 'expected', 'by', 'fall', '2008', 'the', 'ilc', 'engineering', 'design', 'report', 'to', 'be', 'submitted', '... | [-0.03703348055098425, 0.12492715623047129, -0.06429842768504826, 0.0765116402934141, -0.09955781962406011, -0.1925393196105884, 0.015625696539501445, 0.40430474108438086, -0.20683531577278877, -0.3762161851391878, 0.10643603401395547, -0.30834312644768874, 0.01260112741660765, 0.20467423204503027, -0.03764475012818972... |
710.3354 | Exact-exchange energy density in the gauge of a semilocal density
functional approximation | Exact-exchange energy density and energy density of a semilocal density
functional approximation are two key ingredients for modeling the static
correlation, a strongly nonlocal functional of the density, through a local
hybrid functional. Because energy densities are not uniquely defined, the
conventional (Slater) e... | cond-mat.mtrl-sci | exactexchange energy density and energy density of a semilocal density functional approximation are two key ingredients for modeling the static correlation a strongly nonlocal functional of the density through a local hybrid functional because energy densities are not uniquely defined the conventional slater exactexcha... | [['exactexchange', 'energy', 'density', 'and', 'energy', 'density', 'of', 'a', 'semilocal', 'density', 'functional', 'approximation', 'are', 'two', 'key', 'ingredients', 'for', 'modeling', 'the', 'static', 'correlation', 'a', 'strongly', 'nonlocal', 'functional', 'of', 'the', 'density', 'through', 'a', 'local', 'hybrid... | [-0.11415518662671546, 0.08477015791074584, -0.13447599763250245, 0.12776818400564113, 0.0019318765458687173, -0.10284149146626716, 0.01617974435378398, 0.3529806274409684, -0.2404646730971184, -0.2843129336229199, -0.005450905344521554, -0.26233488981091935, -0.1411239115170554, 0.11554277676774503, 0.0219533265290128... |
710.3355 | Lensing Systematics from Space: Modeling PSF effects in the SNAP survey | Anisotropy in the point spread function (PSF) contributes a systematic error
to weak lensing measurements. In this study we use a ray tracer that
incorporates all the optical elements of the SNAP telescope to estimate this
effect. Misalignments in the optics generates PSF anisotropy, which we
characterize by its elli... | astro-ph | anisotropy in the point spread function psf contributes a systematic error to weak lensing measurements in this study we use a ray tracer that incorporates all the optical elements of the snap telescope to estimate this effect misalignments in the optics generates psf anisotropy which we characterize by its ellipticity... | [['anisotropy', 'in', 'the', 'point', 'spread', 'function', 'psf', 'contributes', 'a', 'systematic', 'error', 'to', 'weak', 'lensing', 'measurements', 'in', 'this', 'study', 'we', 'use', 'a', 'ray', 'tracer', 'that', 'incorporates', 'all', 'the', 'optical', 'elements', 'of', 'the', 'snap', 'telescope', 'to', 'estimate'... | [-0.13416044588398787, 0.11494336678009566, -0.07781434923025041, 0.09390260135934249, -0.06576091818907566, -0.03550922283742192, 0.011380312429077324, 0.3861396709649727, -0.2776406464948394, -0.32956956654530145, 0.05650437270202834, -0.31931595251649275, -0.09589855718839882, 0.2302965597442255, -0.0196203831569880... |
710.3356 | Freyd's generating hypothesis for groups with periodic cohomology | Let $G$ be a finite group and let $k$ be a field whose characteristic $p$
divides the order of $G$. Freyd's generating hypothesis for the stable module
category of $G$ is the statement that a map between finite-dimensional
$kG$-modules in the thick subcategory generated by $k$ factors through a
projective if the indu... | math.RT math.AT math.GR | let g be a finite group and let k be a field whose characteristic p divides the order of g freyds generating hypothesis for the stable module category of g is the statement that a map between finitedimensional kgmodules in the thick subcategory generated by k factors through a projective if the induced map on tate coho... | [['let', 'g', 'be', 'a', 'finite', 'group', 'and', 'let', 'k', 'be', 'a', 'field', 'whose', 'characteristic', 'p', 'divides', 'the', 'order', 'of', 'g', 'freyds', 'generating', 'hypothesis', 'for', 'the', 'stable', 'module', 'category', 'of', 'g', 'is', 'the', 'statement', 'that', 'a', 'map', 'between', 'finitedimensio... | [-0.22695372212112097, 0.1477246279463026, -0.12802541504303613, -0.0040160468790917565, -0.10651041926386967, -0.17289688186172178, -0.014454136079282262, 0.3956387923007794, -0.36891554412888544, -0.1936538706341868, 0.07887914067695793, -0.2130511239554514, -0.10653745488711067, 0.1947453475914503, -0.11064674821225... |
710.3357 | Riemann surfaces and AF-algebras | For a generic set in the Teichmueller space, we construct a covariant functor
with the range in a category of the AF-algebras; the functor maps isomorphic
Riemann surfaces to the stably isomorphic AF-algebras. As a special case, one
gets a categorical correspondence between complex tori and the so-called
Effros-Shen ... | math.OA math.AG | for a generic set in the teichmueller space we construct a covariant functor with the range in a category of the afalgebras the functor maps isomorphic riemann surfaces to the stably isomorphic afalgebras as a special case one gets a categorical correspondence between complex tori and the socalled effrosshen algebras | [['for', 'a', 'generic', 'set', 'in', 'the', 'teichmueller', 'space', 'we', 'construct', 'a', 'covariant', 'functor', 'with', 'the', 'range', 'in', 'a', 'category', 'of', 'the', 'afalgebras', 'the', 'functor', 'maps', 'isomorphic', 'riemann', 'surfaces', 'to', 'the', 'stably', 'isomorphic', 'afalgebras', 'as', 'a', 'sp... | [-0.1631657992117107, 0.04993355693295598, -0.08618376798927783, 0.13570642098085955, -0.10088008265942335, -0.13517924952786417, -0.028497994393110276, 0.33532266872003674, -0.39933808129280807, -0.13819505812600255, 0.0955138044198975, -0.23969298254785826, -0.15104295916855334, 0.19506997402757406, -0.19717430671676... |
710.3358 | On $q$-complete and $q$-concave with corners complex manifolds | It is proved that if there exists a positive and continuous function $f$ on an $n$-dimensional complex manifold $X$, $q$-convex with corners outside a compact set $K\subset X$ and which exhausts $X$ from below, then $dim_{\mathbb{C}}H^{p}(X,{\mathcal{F}})<+\infty$ for any coherent analytic sheaf ${\mathcal{F}}$ on $X$ ... | math.CV | it is proved that if there exists a positive and continuous function f on an ndimensional complex manifold x qconvex with corners outside a compact set ksubset x and which exhausts x from below then dim_mathbbchpxmathcalfinfty for any coherent analytic sheaf mathcalf on x if pnq it is known from the theory of andreotti... | [['it', 'is', 'proved', 'that', 'if', 'there', 'exists', 'a', 'positive', 'and', 'continuous', 'function', 'f', 'on', 'an', 'ndimensional', 'complex', 'manifold', 'x', 'qconvex', 'with', 'corners', 'outside', 'a', 'compact', 'set', 'ksubset', 'x', 'and', 'which', 'exhausts', 'x', 'from', 'below', 'then', 'dim_mathbbchp... | [-0.16764619934417488, 0.113851961924597, -0.04831792151342225, 0.03182560999468193, -0.06321972471112049, -0.17808935964053654, 0.004302827088044485, 0.3795004679249173, -0.28022418764324475, -0.1650187253004574, 0.10977392506937171, -0.29590810598463313, -0.15397162157961544, 0.18570305393582368, -0.12925674311581056... |
710.3359 | Generation of Magnetic Field by Combined Action of Turbulence and Shear | The feasibility of a mean-field dynamo in nonhelical turbulence with
superimposed linear shear is studied numerically in elongated shearing boxes.
Exponential growth of magnetic field at scales much larger than the outer scale
of the turbulence is found. The charateristic scale of the field is l_B ~
S^{-1/2} and grow... | astro-ph nlin.CD physics.flu-dyn physics.plasm-ph | the feasibility of a meanfield dynamo in nonhelical turbulence with superimposed linear shear is studied numerically in elongated shearing boxes exponential growth of magnetic field at scales much larger than the outer scale of the turbulence is found the charateristic scale of the field is l_b s12 and growth rate is g... | [['the', 'feasibility', 'of', 'a', 'meanfield', 'dynamo', 'in', 'nonhelical', 'turbulence', 'with', 'superimposed', 'linear', 'shear', 'is', 'studied', 'numerically', 'in', 'elongated', 'shearing', 'boxes', 'exponential', 'growth', 'of', 'magnetic', 'field', 'at', 'scales', 'much', 'larger', 'than', 'the', 'outer', 'sc... | [-0.23548422686607492, 0.23537307850677858, -0.03332505222219466, 0.11142229218438099, -0.0558446107421663, -0.08327396399743686, -0.07882835367821496, 0.2936061207649552, -0.2936240134400908, -0.2662195600992577, 0.06344141830579081, -0.1845057472839306, -0.07002414712438952, 0.2543357872636989, 0.06966727669879963, 0... |
710.336 | Detailed magnetization study of superconducting properties of YBCO
ceramic spheres | We present a magnetization study of low density YBCO ceramics carried out in
magnetic fields 0.5 Oe < H < 50 kOe. It was demonstrated that superconducting
links between grains may be completely suppressed either by a magnetic field of
the order of 100 Oe (at low temperatures) or by an increase of temperature
above 70... | cond-mat.supr-con | we present a magnetization study of low density ybco ceramics carried out in magnetic fields 05 oe h 50 koe it was demonstrated that superconducting links between grains may be completely suppressed either by a magnetic field of the order of 100 oe at low temperatures or by an increase of temperature above 70 k this pr... | [['we', 'present', 'a', 'magnetization', 'study', 'of', 'low', 'density', 'ybco', 'ceramics', 'carried', 'out', 'in', 'magnetic', 'fields', '05', 'oe', 'h', '50', 'koe', 'it', 'was', 'demonstrated', 'that', 'superconducting', 'links', 'between', 'grains', 'may', 'be', 'completely', 'suppressed', 'either', 'by', 'a', 'm... | [-0.1418574156019477, 0.1968691171676273, -0.051140864601008376, -0.025431062771603327, -0.042446909423935975, -0.11208612811152298, 0.12877779301385037, 0.37722588217549835, -0.208644549994001, -0.36256506863870835, 0.027799574280789326, -0.29566018076355355, 0.003922001812560945, 0.21980918938234117, 0.05666579981565... |
710.3361 | Final results on nu_mu to nu_tau oscillation from the CHORUS experiment | The final oscillation analysis of the complete set of data collected by
CHORUS in the years 1994--1997 is presented. Reconstruction algorithms of data
extracted by electronic detectors were improved and the data recorded in the
emulsion target were analysed by new automated scanning systems, allowing the
use of a new... | hep-ex | the final oscillation analysis of the complete set of data collected by chorus in the years 19941997 is presented reconstruction algorithms of data extracted by electronic detectors were improved and the data recorded in the emulsion target were analysed by new automated scanning systems allowing the use of a new metho... | [['the', 'final', 'oscillation', 'analysis', 'of', 'the', 'complete', 'set', 'of', 'data', 'collected', 'by', 'chorus', 'in', 'the', 'years', '19941997', 'is', 'presented', 'reconstruction', 'algorithms', 'of', 'data', 'extracted', 'by', 'electronic', 'detectors', 'were', 'improved', 'and', 'the', 'data', 'recorded', '... | [-0.06660359088952343, 0.12308393363050665, -0.05463426116972586, 0.0775046494152665, -0.00454805510570154, -0.07615395444515867, 0.09451513685935149, 0.31117390468011075, -0.15223395000353004, -0.4241991356918306, 0.09836914248686905, -0.3487626918111787, -0.022276656202986047, 0.2406945411595657, -0.02206585573113636... |
710.3362 | Scale-renormalized matrix-product states for correlated quantum systems | A generalization of matrix product states (MPS) is introduced which is
suitable for describing interacting quantum systems in two and three
dimensions. These scale-renormalized matrix-product states (SR-MPS) are based
on a course-graining of the lattice in which the blocks at each level are
associated with matrix pro... | cond-mat.str-el cond-mat.stat-mech | a generalization of matrix product states mps is introduced which is suitable for describing interacting quantum systems in two and three dimensions these scalerenormalized matrixproduct states srmps are based on a coursegraining of the lattice in which the blocks at each level are associated with matrix products that ... | [['a', 'generalization', 'of', 'matrix', 'product', 'states', 'mps', 'is', 'introduced', 'which', 'is', 'suitable', 'for', 'describing', 'interacting', 'quantum', 'systems', 'in', 'two', 'and', 'three', 'dimensions', 'these', 'scalerenormalized', 'matrixproduct', 'states', 'srmps', 'are', 'based', 'on', 'a', 'coursegra... | [-0.06148433058035814, 0.19615108963440764, -0.07110160644250837, 0.05971171605739404, 0.019884474321522495, -0.14912838620260696, -0.009429561010223221, 0.37653598881919276, -0.2539916785095226, -0.24861288836479864, 0.15159796090076932, -0.2799014985561371, -0.14169778765856542, 0.20526446148710834, 0.061581212332980... |
710.3363 | Using X-ray observations to identify the particle acceleration
mechanisms in VHE SNRs and "dark" VHE sources | Very high energy (VHE) gamma-ray observations have proven to be very
successful in localizing Galactic acceleration sites of VHE particles.
Observations of shell-type supernova remnants have confirmed that particles are
accelerated to VHE energies in supernova blast waves; the interpretation of the
gamma-ray data in ... | astro-ph | very high energy vhe gammaray observations have proven to be very successful in localizing galactic acceleration sites of vhe particles observations of shelltype supernova remnants have confirmed that particles are accelerated to vhe energies in supernova blast waves the interpretation of the gammaray data in terms of ... | [['very', 'high', 'energy', 'vhe', 'gammaray', 'observations', 'have', 'proven', 'to', 'be', 'very', 'successful', 'in', 'localizing', 'galactic', 'acceleration', 'sites', 'of', 'vhe', 'particles', 'observations', 'of', 'shelltype', 'supernova', 'remnants', 'have', 'confirmed', 'that', 'particles', 'are', 'accelerated'... | [-0.048122410234313885, 0.18881862319159343, -0.020136111540932384, 0.17484898100944624, -0.17440215154744734, -0.08992909439433142, 0.011003972847645965, 0.42893252600509446, -0.21260241063424204, -0.38475446364273563, 0.012296188450043384, -0.33533950394407014, 0.04937119218177043, 0.24487877704731295, 0.002103550159... |
710.3364 | Spectral properties of the nonspherically decaying radiation generated
by a rotating superluminal source | The focusing of the radiation generated by a polarization current with a
superluminally rotating distribution pattern is of a higher order in the plane
of rotation than in other directions. Consequently, our previously published
asymptotic approximation to the value of this field outside the equatorial
plane breaks d... | astro-ph | the focusing of the radiation generated by a polarization current with a superluminally rotating distribution pattern is of a higher order in the plane of rotation than in other directions consequently our previously published asymptotic approximation to the value of this field outside the equatorial plane breaks down ... | [['the', 'focusing', 'of', 'the', 'radiation', 'generated', 'by', 'a', 'polarization', 'current', 'with', 'a', 'superluminally', 'rotating', 'distribution', 'pattern', 'is', 'of', 'a', 'higher', 'order', 'in', 'the', 'plane', 'of', 'rotation', 'than', 'in', 'other', 'directions', 'consequently', 'our', 'previously', 'p... | [-0.1423343022201944, 0.16569931757791087, -0.0707504399243858, 0.03176801714628761, -0.08432060600152248, -0.0846237104924135, 0.029128384491595515, 0.3814024155949836, -0.24192573215180305, -0.2781328326419908, 0.10599888542575346, -0.27529257126490303, -0.05867959962556998, 0.20574546778342961, 0.008901573446159458,... |
710.3365 | Singular Yamabe metrics and initial data with exactly
Kottler-Schwarzschild-de Sitter ends | We construct large families of initial data sets for the vacuum Einstein
equations with positive cosmological constant which contain exactly Delaunay
ends; these are non-trivial initial data sets which coincide with those for the
Kottler-Schwarzschild-de Sitter metrics in regions of infinite extent. From the
purely R... | gr-qc math.DG | we construct large families of initial data sets for the vacuum einstein equations with positive cosmological constant which contain exactly delaunay ends these are nontrivial initial data sets which coincide with those for the kottlerschwarzschildde sitter metrics in regions of infinite extent from the purely riemanni... | [['we', 'construct', 'large', 'families', 'of', 'initial', 'data', 'sets', 'for', 'the', 'vacuum', 'einstein', 'equations', 'with', 'positive', 'cosmological', 'constant', 'which', 'contain', 'exactly', 'delaunay', 'ends', 'these', 'are', 'nontrivial', 'initial', 'data', 'sets', 'which', 'coincide', 'with', 'those', 'f... | [-0.15277182815469065, 0.11230234498650117, -0.08904061584188691, 0.09442663039322416, -0.11590163527003858, -0.18646298721432686, -0.08259882689629383, 0.343410189175662, -0.19601101203347152, -0.2627540413720779, 0.11883164714595724, -0.29534380257410825, -0.10065082280966893, 0.17551741536864834, -0.0946575667673968... |
710.3366 | From Quark-Gluon Plasma to the Perfect Liquid | After reviewing some basic concepts of the theory of strongly interacting
matter above nuclear energy density and reviewing some salient results of the
experimental program at the Relativistic Heavy Ion Collider (RHIC), these
lectures explain why the quark-gluon plasma observed in the RHIC experiments
has been called... | nucl-th | after reviewing some basic concepts of the theory of strongly interacting matter above nuclear energy density and reviewing some salient results of the experimental program at the relativistic heavy ion collider rhic these lectures explain why the quarkgluon plasma observed in the rhic experiments has been called a per... | [['after', 'reviewing', 'some', 'basic', 'concepts', 'of', 'the', 'theory', 'of', 'strongly', 'interacting', 'matter', 'above', 'nuclear', 'energy', 'density', 'and', 'reviewing', 'some', 'salient', 'results', 'of', 'the', 'experimental', 'program', 'at', 'the', 'relativistic', 'heavy', 'ion', 'collider', 'rhic', 'thes... | [-0.07132906176742505, 0.2542598078423246, -0.16974008766489782, 0.12148214921101251, -0.06356200160172937, -0.11829780156999319, -0.047298132596717384, 0.30993943904865195, -0.23417032954537056, -0.2810754558092661, 0.043044291604680686, -0.3198626061202958, -0.02795942392020317, 0.11756627372762357, 0.016406532948498... |
710.3367 | Schiff Theorem Revisited | We carefully rederive the Schiff theorem and prove that the usual expression
of the Schiff moment operator is correct and should be applied for calculations
of atomic electric dipole moments. The recently discussed corrections to the
definition of the Schiff moment are absent.
| nucl-th hep-ph hep-th physics.atom-ph | we carefully rederive the schiff theorem and prove that the usual expression of the schiff moment operator is correct and should be applied for calculations of atomic electric dipole moments the recently discussed corrections to the definition of the schiff moment are absent | [['we', 'carefully', 'rederive', 'the', 'schiff', 'theorem', 'and', 'prove', 'that', 'the', 'usual', 'expression', 'of', 'the', 'schiff', 'moment', 'operator', 'is', 'correct', 'and', 'should', 'be', 'applied', 'for', 'calculations', 'of', 'atomic', 'electric', 'dipole', 'moments', 'the', 'recently', 'discussed', 'corr... | [-0.09961965911870085, 0.14828389919861112, -0.047669308779891145, 0.19432211815931855, -0.051079093998428, -0.033754866267012996, 0.03266532789796677, 0.29307997192061225, -0.22008285673638417, -0.2557524112161509, 0.0019750954085137953, -0.2995499728334158, -0.08194617948733098, 0.12848186922302945, -0.00287399137782... |
710.3368 | Local power fluctuations in two-dimensional turbulence | The statistics of power fluctuations are studied in simulations of
two-dimensional turbulence in both inverse (energy) and direct (enstrophy)
cascade regimes from both Lagrangian and Eulerian perspectives. The probability
density function (PDF) of the appropriately defined dimensionless power is
strongly non-gaussian... | cond-mat.stat-mech | the statistics of power fluctuations are studied in simulations of twodimensional turbulence in both inverse energy and direct enstrophy cascade regimes from both lagrangian and eulerian perspectives the probability density function pdf of the appropriately defined dimensionless power is strongly nongaussian with asymm... | [['the', 'statistics', 'of', 'power', 'fluctuations', 'are', 'studied', 'in', 'simulations', 'of', 'twodimensional', 'turbulence', 'in', 'both', 'inverse', 'energy', 'and', 'direct', 'enstrophy', 'cascade', 'regimes', 'from', 'both', 'lagrangian', 'and', 'eulerian', 'perspectives', 'the', 'probability', 'density', 'fun... | [-0.1379834200415644, 0.1450241056219446, -0.1484809845029044, 0.10623858854835687, 0.02310861450470319, -0.08149557561098066, -0.01761595555269326, 0.2801344599242189, -0.29240584548928644, -0.27143740077735856, 0.045436904156563936, -0.298085591090577, -0.0746313786949031, 0.2055220911611936, 0.014568969016961222, 0.... |
710.3369 | Multi-Fluid Simulation of the Magnetic Field Evolution in Neutron Stars | Using a numerical simulation, we study the effects of ambipolar diffusion and
ohmic diffusion on the magnetic field evolution in the interior of an isolated
neutron star. We are interested in the behavior of the magnetic field on a long
time scale, over which all Alfven and sound waves have been damped. We model
the ... | astro-ph | using a numerical simulation we study the effects of ambipolar diffusion and ohmic diffusion on the magnetic field evolution in the interior of an isolated neutron star we are interested in the behavior of the magnetic field on a long time scale over which all alfven and sound waves have been damped we model the stella... | [['using', 'a', 'numerical', 'simulation', 'we', 'study', 'the', 'effects', 'of', 'ambipolar', 'diffusion', 'and', 'ohmic', 'diffusion', 'on', 'the', 'magnetic', 'field', 'evolution', 'in', 'the', 'interior', 'of', 'an', 'isolated', 'neutron', 'star', 'we', 'are', 'interested', 'in', 'the', 'behavior', 'of', 'the', 'ma... | [-0.1625742321111775, 0.24202862498446293, -0.06235713564022584, 0.0471248473514786, -0.035231709597049514, -0.07015874866859062, -0.025768428178598916, 0.37463032767667387, -0.27779319592400226, -0.2958668959410694, 0.03476977999416922, -0.2879855900244442, -0.05714479014368081, 0.158323988958379, 0.07598099602709808,... |
710.337 | The effect of 3He impurities on the nonclassical response to oscillation
of solid 4He | We have investigated the influence of impurities on the possible supersolid
transition by systematically enriching isotopically-pure 4He (< 1 ppb of 3He)
with 3He. The onset of nonclassical rotational inertia is broadened and shifts
monotonically to higher temperature with increasing 3He concentration,
suggesting tha... | cond-mat.other cond-mat.stat-mech | we have investigated the influence of impurities on the possible supersolid transition by systematically enriching isotopicallypure 4he 1 ppb of 3he with 3he the onset of nonclassical rotational inertia is broadened and shifts monotonically to higher temperature with increasing 3he concentration suggesting that the phe... | [['we', 'have', 'investigated', 'the', 'influence', 'of', 'impurities', 'on', 'the', 'possible', 'supersolid', 'transition', 'by', 'systematically', 'enriching', 'isotopicallypure', '4he', '1', 'ppb', 'of', '3he', 'with', '3he', 'the', 'onset', 'of', 'nonclassical', 'rotational', 'inertia', 'is', 'broadened', 'and', 's... | [-0.044046138087287544, 0.3962933922341714, -0.0398366011834393, 0.010881888420165827, 0.07092640449603399, -0.10948404893279076, 0.08536583927537625, 0.3706980840923885, -0.21126384682332475, -0.23090708948050936, -0.07485951916508687, -0.367214853145803, -0.015458992480610808, 0.08800008442873757, 0.03404892383453747... |
710.3371 | Segregation process and phase transition in cyclic predator-prey models
with even number of species | We study a spatial cyclic predator-prey model with an even number of species
(for n=4, 6, and 8) that allows the formation of two defective alliances
consisting of the even and odd label species. The species are distributed on
the sites of a square lattice. The evolution of spatial distribution is
governed by iterati... | physics.bio-ph q-bio.PE | we study a spatial cyclic predatorprey model with an even number of species for n4 6 and 8 that allows the formation of two defective alliances consisting of the even and odd label species the species are distributed on the sites of a square lattice the evolution of spatial distribution is governed by iteration of two ... | [['we', 'study', 'a', 'spatial', 'cyclic', 'predatorprey', 'model', 'with', 'an', 'even', 'number', 'of', 'species', 'for', 'n4', '6', 'and', '8', 'that', 'allows', 'the', 'formation', 'of', 'two', 'defective', 'alliances', 'consisting', 'of', 'the', 'even', 'and', 'odd', 'label', 'species', 'the', 'species', 'are', 'd... | [-0.15858234291902829, 0.2442955165509678, 0.01724384452302194, 0.052343062468264555, 0.05554928710182191, -0.17130614708488187, 0.10232126135511178, 0.37609753585981986, -0.26763103071415256, -0.28041938030497826, 0.06641757415924618, -0.31174564013657646, -0.09663064306947, 0.07630604440313335, 0.04481263663487654, -... |
710.3372 | Non-linearizable Actions of Commutative Reductive Groups | We generalize a construction of Freudenburg and Moser-Jauslin in order to
obtain an example of a non-linearizable action of a commutative reductive
algebraic group on the affine space for every field of characteristic zero
which admits a quadratic field extension.
| math.AG math.RT | we generalize a construction of freudenburg and moserjauslin in order to obtain an example of a nonlinearizable action of a commutative reductive algebraic group on the affine space for every field of characteristic zero which admits a quadratic field extension | [['we', 'generalize', 'a', 'construction', 'of', 'freudenburg', 'and', 'moserjauslin', 'in', 'order', 'to', 'obtain', 'an', 'example', 'of', 'a', 'nonlinearizable', 'action', 'of', 'a', 'commutative', 'reductive', 'algebraic', 'group', 'on', 'the', 'affine', 'space', 'for', 'every', 'field', 'of', 'characteristic', 'ze... | [-0.23727364518130437, 0.0452595532857604, -0.15152534087881064, 0.03559018614200445, -0.17431558539661077, -0.12296674147439308, -0.02140523514782007, 0.2899397520873791, -0.305883209579266, -0.17456942409850085, 0.11957914133568127, -0.19029935399213663, -0.1646405613909547, 0.24251007744803643, -0.11263221520811129,... |
710.3373 | Driven Intrinsic Localized Modes in a Coupled Pendulum Array | Intrinsic localized modes (ILMs), also called discrete breathers, are
directly generated via modulational instability in an array of coupled
pendulums. These ILMs can be stabilized over a range of driver frequencies and
amplitudes. They are characterized by a pi-phase difference between their
center and wings. At hig... | nlin.PS | intrinsic localized modes ilms also called discrete breathers are directly generated via modulational instability in an array of coupled pendulums these ilms can be stabilized over a range of driver frequencies and amplitudes they are characterized by a piphase difference between their center and wings at higher driver... | [['intrinsic', 'localized', 'modes', 'ilms', 'also', 'called', 'discrete', 'breathers', 'are', 'directly', 'generated', 'via', 'modulational', 'instability', 'in', 'an', 'array', 'of', 'coupled', 'pendulums', 'these', 'ilms', 'can', 'be', 'stabilized', 'over', 'a', 'range', 'of', 'driver', 'frequencies', 'and', 'amplit... | [-0.2126743705559741, 0.29434829889578396, -0.05777073545408819, 0.08725906426415724, -0.078786665601108, -0.12601175151683172, 0.012015536102219759, 0.4453234520384713, -0.28991672435008425, -0.2135878923239515, 0.12271958910551962, -0.25900519909063247, -0.15476434887386858, 0.22931125662837396, 0.029433712541290066,... |
710.3374 | An arithmetic Riemann-Roch theorem for pointed stable curves | We prove an arithmetic Riemann-Roch theorem for pointed stable curves. We
derive consequences for the Selberg zeta function of an open modular curve
$Y_{1}(p)$ (resp. $Y_{0}(p)$), for a prime number $p\geq 11$ (resp. congruent
to 11 modulo 12).
| math.NT math.AG | we prove an arithmetic riemannroch theorem for pointed stable curves we derive consequences for the selberg zeta function of an open modular curve y_1p resp y_0p for a prime number pgeq 11 resp congruent to 11 modulo 12 | [['we', 'prove', 'an', 'arithmetic', 'riemannroch', 'theorem', 'for', 'pointed', 'stable', 'curves', 'we', 'derive', 'consequences', 'for', 'the', 'selberg', 'zeta', 'function', 'of', 'an', 'open', 'modular', 'curve', 'y_1p', 'resp', 'y_0p', 'for', 'a', 'prime', 'number', 'pgeq', '11', 'resp', 'congruent', 'to', '11', ... | [-0.2736560449314614, 0.04231332355751268, -0.14995507864902416, 0.17207196251385742, -0.011660658030046357, -0.20865019507861385, 0.058071226204952434, 0.28366514838611084, -0.32093469495238325, -0.2452291666995734, 0.06560459466547602, -0.25405895081348717, -0.1250354092917405, 0.2923603375869182, -0.1748691853653225... |
710.3375 | On the Capacity of Interference Channels with One Cooperating
Transmitter | Inner and outer bounds are established on the capacity region of two-sender,
two-receiver interference channels where one transmitter knows both messages.
The transmitter with extra knowledge is referred to as being cognitive. The
inner bound is based on strategies that generalize prior work, and include
rate-splitti... | cs.IT math.IT | inner and outer bounds are established on the capacity region of twosender tworeceiver interference channels where one transmitter knows both messages the transmitter with extra knowledge is referred to as being cognitive the inner bound is based on strategies that generalize prior work and include ratesplitting gelfan... | [['inner', 'and', 'outer', 'bounds', 'are', 'established', 'on', 'the', 'capacity', 'region', 'of', 'twosender', 'tworeceiver', 'interference', 'channels', 'where', 'one', 'transmitter', 'knows', 'both', 'messages', 'the', 'transmitter', 'with', 'extra', 'knowledge', 'is', 'referred', 'to', 'as', 'being', 'cognitive', ... | [-0.20369184840350382, 0.05313186570801722, -0.05139068351878274, 0.05957145851245651, -0.10862198834037108, -0.3378937027807678, 0.11441537837988587, 0.3265052503926219, -0.21655241611804213, -0.24652081816106713, 0.1405263152912319, -0.2487997356251443, -0.15006377532206958, 0.16186713202986666, -0.12064145572805246,... |
710.3376 | Superfluid density of superconductor-ferromagnet bilayers | We report the first measurements of the effective superfluid density n_S(T)
\propto \lambda^{-2}(T) of Superconductor-Ferromagnet (SC/FM) bilayers, where
\lambda is the effective magnetic field penetration depth. Thin Nb/Ni bilayers
were sputtered in ultrahigh vacuum in quick succession onto oxidized Si
substrates. N... | cond-mat.supr-con | we report the first measurements of the effective superfluid density n_st propto lambda2t of superconductorferromagnet scfm bilayers where lambda is the effective magnetic field penetration depth thin nbni bilayers were sputtered in ultrahigh vacuum in quick succession onto oxidized si substrates nb layers are 102 a th... | [['we', 'report', 'the', 'first', 'measurements', 'of', 'the', 'effective', 'superfluid', 'density', 'n_st', 'propto', 'lambda2t', 'of', 'superconductorferromagnet', 'scfm', 'bilayers', 'where', 'lambda', 'is', 'the', 'effective', 'magnetic', 'field', 'penetration', 'depth', 'thin', 'nbni', 'bilayers', 'were', 'sputter... | [-0.09956706078383067, 0.2734084670941922, 0.007892757055482693, -0.015587674923211572, 0.011224756069067452, -0.17432908459551752, 0.09713826101598522, 0.39614775869625785, -0.2322823598330456, -0.3281723231239806, 0.0017842348629889626, -0.388708999465471, -0.007907052738739857, 0.143190311844505, 0.01327744618590389... |
710.3377 | Transient Random Walks in Random Environment on a Galton-Watson Tree | We consider a transient random walk $(X_n)$ in random environment on a
Galton--Watson tree. Under fairly general assumptions, we give a sharp and
explicit criterion for the asymptotic speed to be positive. As a consequence,
situations with zero speed are revealed to occur. In such cases, we prove that
$X_n$ is of ord... | math.PR | we consider a transient random walk x_n in random environment on a galtonwatson tree under fairly general assumptions we give a sharp and explicit criterion for the asymptotic speed to be positive as a consequence situations with zero speed are revealed to occur in such cases we prove that x_n is of order of magnitude ... | [['we', 'consider', 'a', 'transient', 'random', 'walk', 'x_n', 'in', 'random', 'environment', 'on', 'a', 'galtonwatson', 'tree', 'under', 'fairly', 'general', 'assumptions', 'we', 'give', 'a', 'sharp', 'and', 'explicit', 'criterion', 'for', 'the', 'asymptotic', 'speed', 'to', 'be', 'positive', 'as', 'a', 'consequence',... | [-0.16082084280991016, 0.18386758388518248, -0.10481717229041077, 0.03659124787745261, -0.05145878099489871, -0.16013452056037306, 0.0928130500061914, 0.4187404589164396, -0.2513763237105639, -0.18954329041839946, 0.12447940252943311, -0.25046896666483304, -0.17344739331950454, 0.18088037966815537, -0.09272131613769763... |
710.3378 | Simu-LC : a Light-Curve simulator for CoRoT | Simulating the data that a space instrument like COROT will provide might
look presomptuous. Indeed, it is certainly, when comparing to previous
comparable instruments like IPHIR or GOLF. These two examples show that the
nominal behaviour of the instrument is not always reached, but this does not
prevent this instrum... | astro-ph | simulating the data that a space instrument like corot will provide might look presomptuous indeed it is certainly when comparing to previous comparable instruments like iphir or golf these two examples show that the nominal behaviour of the instrument is not always reached but this does not prevent this instrument to ... | [['simulating', 'the', 'data', 'that', 'a', 'space', 'instrument', 'like', 'corot', 'will', 'provide', 'might', 'look', 'presomptuous', 'indeed', 'it', 'is', 'certainly', 'when', 'comparing', 'to', 'previous', 'comparable', 'instruments', 'like', 'iphir', 'or', 'golf', 'these', 'two', 'examples', 'show', 'that', 'the',... | [-0.10192459061404355, 0.13152667652198186, -0.15523400610009355, 0.11298553573276346, -0.1506932703542701, -0.1413262170671454, 0.02141806467964701, 0.37539191068976785, -0.22460124097317144, -0.36530590279477787, 0.1623645811204359, -0.2719478099031395, -0.13070340924163798, 0.28011575355351476, -0.09394652792129972,... |
710.3379 | Asymptotic description of solitary wave trains in fully nonlinear
shallow-water theory | We derive an asymptotic formula for the amplitude distribution in a fully
nonlinear shallow-water solitary wave train which is formed as the long-time
outcome of the initial-value problem for the Su-Gardner (or one-dimensional
Green-Naghdi) system. Our analysis is based on the properties of the
characteristics of the... | nlin.PS | we derive an asymptotic formula for the amplitude distribution in a fully nonlinear shallowwater solitary wave train which is formed as the longtime outcome of the initialvalue problem for the sugardner or onedimensional greennaghdi system our analysis is based on the properties of the characteristics of the associated... | [['we', 'derive', 'an', 'asymptotic', 'formula', 'for', 'the', 'amplitude', 'distribution', 'in', 'a', 'fully', 'nonlinear', 'shallowwater', 'solitary', 'wave', 'train', 'which', 'is', 'formed', 'as', 'the', 'longtime', 'outcome', 'of', 'the', 'initialvalue', 'problem', 'for', 'the', 'sugardner', 'or', 'onedimensional'... | [-0.1394578581165969, 0.06425973409156638, -0.13283098772098886, 0.06415790026480224, -0.09552599880690417, -0.12070146956565705, -0.08277639203266171, 0.29713832679366275, -0.2818540944814035, -0.21685039926289526, 0.14613569643221458, -0.26920207863873685, -0.18542897805748584, 0.23890001369901925, 0.0100164839551468... |
710.338 | CNI polarimetry with Helium 3 | By making use of previous analysis of CNI for pp and pC scattering, the
spin-flip factor for np scattering is determined as a function of energy and
then used to calculate the p He3 asymmetry A_N(s)' arising in p He 3 elastic
scattering. It is found to be comparable to A_N(s) for pp scattering, but of
the opposite si... | hep-ph nucl-ex | by making use of previous analysis of cni for pp and pc scattering the spinflip factor for np scattering is determined as a function of energy and then used to calculate the p he3 asymmetry a_ns arising in p he 3 elastic scattering it is found to be comparable to a_ns for pp scattering but of the opposite sign it seems... | [['by', 'making', 'use', 'of', 'previous', 'analysis', 'of', 'cni', 'for', 'pp', 'and', 'pc', 'scattering', 'the', 'spinflip', 'factor', 'for', 'np', 'scattering', 'is', 'determined', 'as', 'a', 'function', 'of', 'energy', 'and', 'then', 'used', 'to', 'calculate', 'the', 'p', 'he3', 'asymmetry', 'a_ns', 'arising', 'in'... | [-0.07958845297597643, 0.1653892427045656, -0.10934528997045402, 0.10097560643886314, -0.026338648283854127, -0.14236891903228274, 0.017272808785109145, 0.34432732756862316, -0.3001494094190237, -0.2895418279191577, 0.01646649215437815, -0.31111693752341363, -0.05015390759064375, 0.18606998363822258, 0.0567817003343646... |
710.3381 | An X-ray emitting black hole in a globular cluster | We present optical and X-ray data for the first object showing strong
evidence for being a black hole in a globular cluster. We show the initial
X-ray light curve and X-ray spectrum which led to the discovery that this is an
extremely bright, highly variable source, and thus must be a black hole. We
present the optic... | astro-ph | we present optical and xray data for the first object showing strong evidence for being a black hole in a globular cluster we show the initial xray light curve and xray spectrum which led to the discovery that this is an extremely bright highly variable source and thus must be a black hole we present the optical spectr... | [['we', 'present', 'optical', 'and', 'xray', 'data', 'for', 'the', 'first', 'object', 'showing', 'strong', 'evidence', 'for', 'being', 'a', 'black', 'hole', 'in', 'a', 'globular', 'cluster', 'we', 'show', 'the', 'initial', 'xray', 'light', 'curve', 'and', 'xray', 'spectrum', 'which', 'led', 'to', 'the', 'discovery', 't... | [-0.08218651009053829, 0.050079535695873305, -0.09473910988465453, 0.09564182030042277, -0.12246517843326156, -0.12413641380857718, 0.0811534819423399, 0.4573457541593005, -0.2226865177913935, -0.30138556297156915, 0.12416582579562294, -0.310474058048109, -0.07301825330477585, 0.2610768869707591, -0.02379660132560837, ... |
710.3382 | Electron spin relaxation via flexural phonon modes in semiconducting
carbon nanotubes | This work considers the g-tensor anisotropy induced by the flexural thermal
vibrations in one-dimensional structures and its role in electron spin
relaxation. In particular, the mechanism of spin-lattice relaxation via
flexural modes is studied theoretically for localized and delocalized
electronic states in semicond... | cond-mat.mtrl-sci | this work considers the gtensor anisotropy induced by the flexural thermal vibrations in onedimensional structures and its role in electron spin relaxation in particular the mechanism of spinlattice relaxation via flexural modes is studied theoretically for localized and delocalized electronic states in semiconducting ... | [['this', 'work', 'considers', 'the', 'gtensor', 'anisotropy', 'induced', 'by', 'the', 'flexural', 'thermal', 'vibrations', 'in', 'onedimensional', 'structures', 'and', 'its', 'role', 'in', 'electron', 'spin', 'relaxation', 'in', 'particular', 'the', 'mechanism', 'of', 'spinlattice', 'relaxation', 'via', 'flexural', 'm... | [-0.16590263429854032, 0.2594858289489316, 0.010279159017830577, 0.002724646988231415, 0.01714969361320329, -0.11557146959786868, 0.04102756788468578, 0.44340023331535167, -0.2861592926077035, -0.26769006782426286, -0.004005370245705175, -0.2658407348088729, -0.07462857603135271, 0.16654072400246167, 0.0974252769548414... |
710.3383 | Simultaneous Multi-Wavelength Observations of Magnetic Activity in
Ultracool Dwarfs. II. Mixed Trends in VB10 and LSR1835+32 and the Possible
Role of Rotation | [Abridged] As part of our on-going investigation of magnetic activity in
ultracool dwarfs we present simultaneous radio, X-ray, UV, and optical
observations of LSR1835+32 (M8.5), and simultaneous X-ray and UV observations
of VB10 (M8), both with a duration of about 9 hours. LSR1835+32 exhibits
persistent radio emissi... | astro-ph | abridged as part of our ongoing investigation of magnetic activity in ultracool dwarfs we present simultaneous radio xray uv and optical observations of lsr183532 m85 and simultaneous xray and uv observations of vb10 m8 both with a duration of about 9 hours lsr183532 exhibits persistent radio emission and halpha variab... | [['abridged', 'as', 'part', 'of', 'our', 'ongoing', 'investigation', 'of', 'magnetic', 'activity', 'in', 'ultracool', 'dwarfs', 'we', 'present', 'simultaneous', 'radio', 'xray', 'uv', 'and', 'optical', 'observations', 'of', 'lsr183532', 'm85', 'and', 'simultaneous', 'xray', 'and', 'uv', 'observations', 'of', 'vb10', 'm... | [-0.08643740493027548, 0.16937546753732446, -0.022263880652531872, 0.11276842964843704, -0.08431360434764575, -0.06501292279092119, 0.05921710524189687, 0.4858067670469954, -0.12625317007344025, -0.3665748404986463, 0.08469096831399539, -0.2972240893135823, -0.06167171023663704, 0.22769995438475435, -0.0264193215730334... |
710.3384 | Spitzer Constraints on the Stellar Populations of Lyman-Alpha Emitting
Galaxies at z = 3.1 | We investigate the stellar populations of a sample of 162 Lyman-alpha
emitting galaxies (LAEs) at z = 3.1 in the Extended Chandra Deep Field South,
using deep Spitzer IRAC data available from the GOODS and SIMPLE surveys to
derive reliable stellar population estimates. We divide the LAEs according to
their rest-frame... | astro-ph | we investigate the stellar populations of a sample of 162 lymanalpha emitting galaxies laes at z 31 in the extended chandra deep field south using deep spitzer irac data available from the goods and simple surveys to derive reliable stellar population estimates we divide the laes according to their restframe nearir lum... | [['we', 'investigate', 'the', 'stellar', 'populations', 'of', 'a', 'sample', 'of', '162', 'lymanalpha', 'emitting', 'galaxies', 'laes', 'at', 'z', '31', 'in', 'the', 'extended', 'chandra', 'deep', 'field', 'south', 'using', 'deep', 'spitzer', 'irac', 'data', 'available', 'from', 'the', 'goods', 'and', 'simple', 'survey... | [0.008017596380757483, 0.13007821277254045, -0.06760616214369755, 0.15492743960289695, -0.10783153821781309, -0.0475763517364828, 0.10218238754403162, 0.5022045385281918, -0.022932968243968406, -0.3963991318695184, -0.0028916842987863505, -0.306000022142652, 0.015130699858349606, 0.1715048042068378, -0.0309793542640409... |
710.3385 | Molecular Recollision Interferometry in High Harmonic Generation | We use extreme-ultraviolet interferometry to measure the phase of high-order
harmonic generation from transiently aligned CO2 molecules. We unambiguously
observe a reversal in phase of the high order harmonic emission for higher
harmonic orders with a sufficient degree of alignment. This results from
molecular-scale ... | physics.atom-ph physics.optics | we use extremeultraviolet interferometry to measure the phase of highorder harmonic generation from transiently aligned co2 molecules we unambiguously observe a reversal in phase of the high order harmonic emission for higher harmonic orders with a sufficient degree of alignment this results from molecularscale quantum... | [['we', 'use', 'extremeultraviolet', 'interferometry', 'to', 'measure', 'the', 'phase', 'of', 'highorder', 'harmonic', 'generation', 'from', 'transiently', 'aligned', 'co2', 'molecules', 'we', 'unambiguously', 'observe', 'a', 'reversal', 'in', 'phase', 'of', 'the', 'high', 'order', 'harmonic', 'emission', 'for', 'highe... | [-0.11868841976619664, 0.14618084575997387, -0.07285169823573226, 0.06295634687783411, 0.0009649692976896742, -0.0744469312505912, 0.05195866087121905, 0.40463748566015106, -0.2487330759455145, -0.2656906818803884, 0.007381082536133452, -0.3076083221950824, -0.1425679314972223, 0.1823909493488779, 0.07503132728975168, ... |
710.3386 | Priority diffusion model in lattices and complex networks | We introduce a model for diffusion of two classes of particles ($A$ and $B$)
with priority: where both species are present in the same site the motion of
$A$'s takes precedence over that of $B$'s. This describes realistic situations
in wireless and communication networks. In regular lattices the diffusion of
the two ... | cond-mat.stat-mech cond-mat.dis-nn | we introduce a model for diffusion of two classes of particles a and b with priority where both species are present in the same site the motion of as takes precedence over that of bs this describes realistic situations in wireless and communication networks in regular lattices the diffusion of the two species is normal... | [['we', 'introduce', 'a', 'model', 'for', 'diffusion', 'of', 'two', 'classes', 'of', 'particles', 'a', 'and', 'b', 'with', 'priority', 'where', 'both', 'species', 'are', 'present', 'in', 'the', 'same', 'site', 'the', 'motion', 'of', 'as', 'takes', 'precedence', 'over', 'that', 'of', 'bs', 'this', 'describes', 'realisti... | [-0.17831097228570716, 0.22529951618539532, 0.009770213866105942, -0.01190056416046208, 0.015070290528863335, -0.15233398369624654, 0.0678218227103978, 0.33407021790687275, -0.2650210384797277, -0.2806537738278397, 0.02104929163739252, -0.2988140894848951, -0.10071926139322902, 0.09404479261181915, -0.00517000929355176... |
710.3387 | Energy Dependence of the Delta Resonance: Chiral Dynamics in Action | There is an important connection between the low energy theorems of QCD and
the energy dependence of the Delta resonance in pi-N scattering, as well as the
closely related gamma^{*} N -> pi N reaction. The resonance shape is due not
only to the strong pi-N interaction in the p wave but the small interaction in
the s ... | hep-ph hep-ex nucl-ex nucl-th | there is an important connection between the low energy theorems of qcd and the energy dependence of the delta resonance in pin scattering as well as the closely related gamma n pi n reaction the resonance shape is due not only to the strong pin interaction in the p wave but the small interaction in the s wave the latt... | [['there', 'is', 'an', 'important', 'connection', 'between', 'the', 'low', 'energy', 'theorems', 'of', 'qcd', 'and', 'the', 'energy', 'dependence', 'of', 'the', 'delta', 'resonance', 'in', 'pin', 'scattering', 'as', 'well', 'as', 'the', 'closely', 'related', 'gamma', 'n', 'pi', 'n', 'reaction', 'the', 'resonance', 'sha... | [-0.16002815766209413, 0.2136387200787241, -0.07151020900741771, 0.10017022106330842, -0.07813449541319405, -0.10489862968477057, 0.0037122018946557428, 0.30490599722479994, -0.2403830626534055, -0.2601804162335137, 0.039166511982962816, -0.3105551677695273, -0.12843520987434717, 0.08996374474372715, 0.0551913825240816... |
710.3388 | On the terminal velocity of sedimenting particles in a flowing fluid | The influence of an underlying carrier flow on the terminal velocity of
sedimenting particles is investigated both analytically and numerically. Our
theoretical framework works for a general class of (laminar or turbulent)
velocity fields and, by means of an ordinary perturbation expansion at small
Stokes number, lea... | nlin.CD | the influence of an underlying carrier flow on the terminal velocity of sedimenting particles is investigated both analytically and numerically our theoretical framework works for a general class of laminar or turbulent velocity fields and by means of an ordinary perturbation expansion at small stokes number leads to c... | [['the', 'influence', 'of', 'an', 'underlying', 'carrier', 'flow', 'on', 'the', 'terminal', 'velocity', 'of', 'sedimenting', 'particles', 'is', 'investigated', 'both', 'analytically', 'and', 'numerically', 'our', 'theoretical', 'framework', 'works', 'for', 'a', 'general', 'class', 'of', 'laminar', 'or', 'turbulent', 'v... | [-0.1453441462778001, 0.12703119292935763, -0.03255273664786302, 0.02334104780119889, -0.06665889881898035, -0.09882521396502852, -0.027615473246538735, 0.3074706833644899, -0.30080311869251286, -0.27312651735314347, 0.10826839275777023, -0.2534628864712121, -0.12540593732673516, 0.22793307194753767, 0.0094891567020974... |
710.3389 | Positivity of Tur\'an determinants for orthogonal polynomials | The orthogonal polynomials $p_n$ satisfy Tur\'an's inequality if
$p_n^2(x)-p_{n-1}(x)p_{n+1}(x)\ge 0$ for $n\ge 1$ and for all $x$ in the
interval of orthogonality. We give general criteria for orthogonal polynomials
to satisfy Tur\'an's inequality. This yields the known results for classical
orthogonal polynomials a... | math.CA | the orthogonal polynomials p_n satisfy turans inequality if p_n2xp_n1xp_n1xge 0 for nge 1 and for all x in the interval of orthogonality we give general criteria for orthogonal polynomials to satisfy turans inequality this yields the known results for classical orthogonal polynomials as well as new results for example ... | [['the', 'orthogonal', 'polynomials', 'p_n', 'satisfy', 'turans', 'inequality', 'if', 'p_n2xp_n1xp_n1xge', '0', 'for', 'nge', '1', 'and', 'for', 'all', 'x', 'in', 'the', 'interval', 'of', 'orthogonality', 'we', 'give', 'general', 'criteria', 'for', 'orthogonal', 'polynomials', 'to', 'satisfy', 'turans', 'inequality', '... | [-0.16149730672343418, 0.05843952586516165, -0.05365956434980035, 0.09569789398273525, -0.07042495002791, -0.24472541415777344, 0.011118739915008728, 0.31098449280342233, -0.28823730234916395, -0.19256650015281943, 0.12084950244304939, -0.23533440517404905, -0.13752717048359606, 0.25400640489533544, -0.0940196148406427... |
710.339 | Efficient algorithms for rigid body integration using optimized
splitting methods and exact free rotational motion | Hamiltonian splitting methods are an established technique to derive stable
and accurate integration schemes in molecular dynamics, in which additional
accuracy can be gained using force gradients. For rigid bodies, a tradition
exists in the literature to further split up the kinetic part of the
Hamiltonian, which lo... | cond-mat.stat-mech cond-mat.soft | hamiltonian splitting methods are an established technique to derive stable and accurate integration schemes in molecular dynamics in which additional accuracy can be gained using force gradients for rigid bodies a tradition exists in the literature to further split up the kinetic part of the hamiltonian which lowers t... | [['hamiltonian', 'splitting', 'methods', 'are', 'an', 'established', 'technique', 'to', 'derive', 'stable', 'and', 'accurate', 'integration', 'schemes', 'in', 'molecular', 'dynamics', 'in', 'which', 'additional', 'accuracy', 'can', 'be', 'gained', 'using', 'force', 'gradients', 'for', 'rigid', 'bodies', 'a', 'tradition... | [-0.11390934846837938, 0.06359935282889637, -0.0843123308682282, 0.08249321942151125, -0.05531475530671222, -0.13013250293941903, 0.06597177234943956, 0.4134511411988309, -0.23704593137538593, -0.3406077969287123, 0.09622280498317975, -0.21331783620906727, -0.08692323945994888, 0.23930085632850284, -0.05240504725703171... |
710.3391 | Calabi-Yau Frobenius algebras | We define Calabi-Yau and periodic Frobenius algebras over arbitrary base
commutative rings. We define a Hochschild analogue of Tate cohomology, and show
that the "stable Hochschild cohomology" of periodic CY Frobenius algebras has a
Batalin-Vilkovisky and Frobenius algebra structure. Such algebras include
(centrally ... | math.RA | we define calabiyau and periodic frobenius algebras over arbitrary base commutative rings we define a hochschild analogue of tate cohomology and show that the stable hochschild cohomology of periodic cy frobenius algebras has a batalinvilkovisky and frobenius algebra structure such algebras include centrally extended p... | [['we', 'define', 'calabiyau', 'and', 'periodic', 'frobenius', 'algebras', 'over', 'arbitrary', 'base', 'commutative', 'rings', 'we', 'define', 'a', 'hochschild', 'analogue', 'of', 'tate', 'cohomology', 'and', 'show', 'that', 'the', 'stable', 'hochschild', 'cohomology', 'of', 'periodic', 'cy', 'frobenius', 'algebras', ... | [-0.20676765375044512, -0.018565497286144202, -0.12006379406646651, 0.1532600766977185, -0.16109351693431578, -0.17997099186088575, -0.09584124953687286, 0.3356224105582904, -0.46763769627580326, -0.15376627377344895, 0.12333258971970497, -0.15430128458350645, -0.1915254679279623, 0.13174914390290693, -0.28921831810799... |
710.3392 | Differential operators and BV structures in noncommutative geometry | We introduce a new formalism of differential operators for a general
associative algebra A. It replaces Grothendieck's notion of differential
operator on a commutative algebra in such a way that derivations of the
commutative algebra are replaced by DDer(A), the bimodule of double
derivations. Our differential operat... | math.QA math.AG math.RA | we introduce a new formalism of differential operators for a general associative algebra a it replaces grothendiecks notion of differential operator on a commutative algebra in such a way that derivations of the commutative algebra are replaced by ddera the bimodule of double derivations our differential operators act ... | [['we', 'introduce', 'a', 'new', 'formalism', 'of', 'differential', 'operators', 'for', 'a', 'general', 'associative', 'algebra', 'a', 'it', 'replaces', 'grothendiecks', 'notion', 'of', 'differential', 'operator', 'on', 'a', 'commutative', 'algebra', 'in', 'such', 'a', 'way', 'that', 'derivations', 'of', 'the', 'commut... | [-0.163496966477053, 0.047208793052839544, -0.11985980685158382, 0.11568174587248578, -0.15609137393767014, -0.1381816030238351, -0.039593228668892616, 0.3087066433937201, -0.3713937778430024, -0.1798351132464683, 0.08194535009931984, -0.23262562032542983, -0.19458790302698342, 0.22314836549625364, -0.1838171437387091,... |
710.3393 | Search for New Physics with Photons at the Tevatron | We report on a search for compositeness in ee+gamma events and a search for
gauge-mediated supersymmetry in gamma+gamma+met events. We also report on two
signature-based searches for anomalous production of gamma + gamma + X (where
X=e, mu, gamma, met) and gamma + lepton + X. The analyses are based on 0.9--1.2
fb-1 o... | hep-ex | we report on a search for compositeness in eegamma events and a search for gaugemediated supersymmetry in gammagammamet events we also report on two signaturebased searches for anomalous production of gamma gamma x where xe mu gamma met and gamma lepton x the analyses are based on 0912 fb1 of data from ppbar collisions... | [['we', 'report', 'on', 'a', 'search', 'for', 'compositeness', 'in', 'eegamma', 'events', 'and', 'a', 'search', 'for', 'gaugemediated', 'supersymmetry', 'in', 'gammagammamet', 'events', 'we', 'also', 'report', 'on', 'two', 'signaturebased', 'searches', 'for', 'anomalous', 'production', 'of', 'gamma', 'gamma', 'x', 'whe... | [-0.05741480927431036, 0.1834361918176277, -0.0877308066509947, 0.13745174714941769, -0.05290991991546146, -0.12994400309280882, 0.06832771165933035, 0.3620746165891237, -0.1261140172475878, -0.34261413130767737, 0.009537384264713412, -0.4597552195780828, 0.08675560102904145, 0.17347585988124903, 0.10376669864960109, 0... |
710.3394 | On the systematics of asteroseismological mass determinations of PG1159
stars | We analyze systematics in the asteroseismological mass determination methods
in pulsating PG 1159 stars. We compare the seismic masses resulting from the
comparison of the observed mean period spacings with the usually adopted
asymptotic period spacings, and the average of the computed period spacings.
Computations a... | astro-ph | we analyze systematics in the asteroseismological mass determination methods in pulsating pg 1159 stars we compare the seismic masses resulting from the comparison of the observed mean period spacings with the usually adopted asymptotic period spacings and the average of the computed period spacings computations are ba... | [['we', 'analyze', 'systematics', 'in', 'the', 'asteroseismological', 'mass', 'determination', 'methods', 'in', 'pulsating', 'pg', '1159', 'stars', 'we', 'compare', 'the', 'seismic', 'masses', 'resulting', 'from', 'the', 'comparison', 'of', 'the', 'observed', 'mean', 'period', 'spacings', 'with', 'the', 'usually', 'ado... | [-0.058867166722509065, 0.16554262528674793, -0.1098768367158449, 0.10865334886136743, -0.07274425574867739, -0.05225019700993589, 0.13558524954895684, 0.38165999592497607, -0.139808454563957, -0.3593039566408948, 0.08317918231445075, -0.2460600540068561, -0.02953398885405333, 0.22105601959267243, -0.06698621125986516,... |
710.3395 | If LHC is a Mini-Time-Machines Factory, Can We Notice? | Assuming the hypothesis of TeV-scale multi-dimensional gravity, one can
imagine that at LHC not only mini-black-holes (MBH) will be intensively
created, but also other exotic gravitational configurations, including
hypothetical mini-time-machines (MTM). Like MBH, they should quickly evaporate,
but one can wonder if t... | hep-th gr-qc hep-ph | assuming the hypothesis of tevscale multidimensional gravity one can imagine that at lhc not only miniblackholes mbh will be intensively created but also other exotic gravitational configurations including hypothetical minitimemachines mtm like mbh they should quickly evaporate but one can wonder if their temporal exis... | [['assuming', 'the', 'hypothesis', 'of', 'tevscale', 'multidimensional', 'gravity', 'one', 'can', 'imagine', 'that', 'at', 'lhc', 'not', 'only', 'miniblackholes', 'mbh', 'will', 'be', 'intensively', 'created', 'but', 'also', 'other', 'exotic', 'gravitational', 'configurations', 'including', 'hypothetical', 'minitimemac... | [-0.10480748878470963, 0.2716420850937523, -0.0924242582085995, 0.12982637199999417, -0.0934942655612604, -0.17405413065531875, 0.028654472203431966, 0.33501441076945115, -0.27007629816870254, -0.3107375669356246, 0.04612275387034199, -0.26177579903775183, -0.007299170266352804, 0.14931867476342256, -0.0080055509743906... |
710.3396 | The Zero Age Main Sequence of WIMP burners | We modify a stellar structure code to estimate the effect upon the main
sequence of the accretion of weakly interacting dark matter onto stars and its
subsequent annihilation. The effect upon the stars depends upon whether the
energy generation rate from dark matter annihilation is large enough to shut
off the nuclea... | astro-ph hep-ph | we modify a stellar structure code to estimate the effect upon the main sequence of the accretion of weakly interacting dark matter onto stars and its subsequent annihilation the effect upon the stars depends upon whether the energy generation rate from dark matter annihilation is large enough to shut off the nuclear b... | [['we', 'modify', 'a', 'stellar', 'structure', 'code', 'to', 'estimate', 'the', 'effect', 'upon', 'the', 'main', 'sequence', 'of', 'the', 'accretion', 'of', 'weakly', 'interacting', 'dark', 'matter', 'onto', 'stars', 'and', 'its', 'subsequent', 'annihilation', 'the', 'effect', 'upon', 'the', 'stars', 'depends', 'upon',... | [-0.04212030057848512, 0.21556031717882146, -0.11215586283090194, 0.14384717792895893, -0.16070930118760549, -0.07321369931776459, 0.0642020481473154, 0.3914149456664803, -0.2178677557050947, -0.3329904926610803, 0.07633817268766492, -0.2753096655245841, -0.03884688840938849, 0.19511088382958722, -0.05293216872923663, ... |
710.3397 | Seventy Years of the EPR Paradox | In spite of the fact that statistical predictions of quantum theory (QT) can
only be tested if large amount of data is available a claim has been made that
QT provides the most complete description of an individual physical system.
Einstein's opposition to this claim and the paradox he presented in the article
writte... | quant-ph | in spite of the fact that statistical predictions of quantum theory qt can only be tested if large amount of data is available a claim has been made that qt provides the most complete description of an individual physical system einsteins opposition to this claim and the paradox he presented in the article written toge... | [['in', 'spite', 'of', 'the', 'fact', 'that', 'statistical', 'predictions', 'of', 'quantum', 'theory', 'qt', 'can', 'only', 'be', 'tested', 'if', 'large', 'amount', 'of', 'data', 'is', 'available', 'a', 'claim', 'has', 'been', 'made', 'that', 'qt', 'provides', 'the', 'most', 'complete', 'description', 'of', 'an', 'indi... | [-0.08667560084143755, 0.13194003920618153, -0.11304779788531336, 0.0981749006018821, -0.08791890013059463, -0.18697357614204954, 0.04116304670993368, 0.3262553111145004, -0.23060389550997723, -0.3102934160061292, 0.03808858198639636, -0.2871834525180545, -0.13954282405934487, 0.20433867617280904, -0.07577777889427446,... |
710.3398 | Simple derivation of the special theory of relativity without the speed
of light axiom | We show a very simple yet rigorous derivation of the invariance of the
space-time interval (and hence the whole special relativity) just from the
isotropy, homogeneity and a principle of relativity, without the need of the
speed of light axiom. This article is intended as a textbook explanation of the
special relativ... | physics.class-ph | we show a very simple yet rigorous derivation of the invariance of the spacetime interval and hence the whole special relativity just from the isotropy homogeneity and a principle of relativity without the need of the speed of light axiom this article is intended as a textbook explanation of the special relativity | [['we', 'show', 'a', 'very', 'simple', 'yet', 'rigorous', 'derivation', 'of', 'the', 'invariance', 'of', 'the', 'spacetime', 'interval', 'and', 'hence', 'the', 'whole', 'special', 'relativity', 'just', 'from', 'the', 'isotropy', 'homogeneity', 'and', 'a', 'principle', 'of', 'relativity', 'without', 'the', 'need', 'of',... | [-0.1357931658052481, 0.06979182335691383, -0.14841903236587173, 0.11265437741978811, -0.16853500891906711, -0.1505894274182188, 0.06622839380333272, 0.284012396255723, -0.23456682734048137, -0.28984305534798366, 0.0927238604053855, -0.15913637400640604, -0.11780547415121244, 0.18433502746316102, -0.0995941951763458, 0... |
710.3399 | From Solar and Stellar Flares to Coronal Heating: Theory and
Observations of How Magnetic Reconnection Regulates Coronal Conditions | There is currently no explanation of why the corona has the temperature and
density it has. We present a model which explains how the dynamics of magnetic
reconnection regulates the conditions in the corona. A bifurcation in magnetic
reconnection at a critical state enforces an upper bound on the coronal
temperature ... | astro-ph physics.plasm-ph physics.space-ph | there is currently no explanation of why the corona has the temperature and density it has we present a model which explains how the dynamics of magnetic reconnection regulates the conditions in the corona a bifurcation in magnetic reconnection at a critical state enforces an upper bound on the coronal temperature for ... | [['there', 'is', 'currently', 'no', 'explanation', 'of', 'why', 'the', 'corona', 'has', 'the', 'temperature', 'and', 'density', 'it', 'has', 'we', 'present', 'a', 'model', 'which', 'explains', 'how', 'the', 'dynamics', 'of', 'magnetic', 'reconnection', 'regulates', 'the', 'conditions', 'in', 'the', 'corona', 'a', 'bifu... | [-0.14975642260891953, 0.22308393474283558, -0.051483547207952916, 0.15109729460686788, -0.04751884737908412, -0.05030079977051623, 0.07773867169737644, 0.3486896330148153, -0.15009016930607372, -0.34050086832166404, 0.07447319034749278, -0.2536985034487028, -0.1281316420384522, 0.21592207361633578, -0.0348892317678051... |
710.34 | Intra Cluster Globular Clusters around NGC 1399 in Fornax? | We investigate whether the globular clusters (GCs) in the recently published
sample of GCs in the Fornax cluster by Bergond and coworkers are indeed
intra-cluster objects. We combine the catalogue of radial velocity measurements
by Bergond et al. with our CTIO MOSAIC photometry in the Washington system and
analyse th... | astro-ph | we investigate whether the globular clusters gcs in the recently published sample of gcs in the fornax cluster by bergond and coworkers are indeed intracluster objects we combine the catalogue of radial velocity measurements by bergond et al with our ctio mosaic photometry in the washington system and analyse the relat... | [['we', 'investigate', 'whether', 'the', 'globular', 'clusters', 'gcs', 'in', 'the', 'recently', 'published', 'sample', 'of', 'gcs', 'in', 'the', 'fornax', 'cluster', 'by', 'bergond', 'and', 'coworkers', 'are', 'indeed', 'intracluster', 'objects', 'we', 'combine', 'the', 'catalogue', 'of', 'radial', 'velocity', 'measur... | [-0.04986554335725183, 0.0731241897738073, -0.13444927350307503, 0.06910093483609325, -0.13628944530223852, -0.05262324701262904, 0.042451371453353204, 0.4439993354109382, -0.12492544453250178, -0.37868557277224246, -0.0264045991047862, -0.30082914215468226, -0.02501406853913241, 0.1981899687407782, -0.0643748124753723... |
710.3401 | Duality, Vector advection and the Navier-Stokes equations | In this article we show that three dimensional vector advection equation is
self dual in certain sense defined below. As a consequence, we infer classical
result of Serrin of existence of strong solution of Navier-Stokes equation.
Also we deduce Feynman-Kac type formula for solution of the vector advection
equation a... | math.PR math.AP | in this article we show that three dimensional vector advection equation is self dual in certain sense defined below as a consequence we infer classical result of serrin of existence of strong solution of navierstokes equation also we deduce feynmankac type formula for solution of the vector advection equation and show... | [['in', 'this', 'article', 'we', 'show', 'that', 'three', 'dimensional', 'vector', 'advection', 'equation', 'is', 'self', 'dual', 'in', 'certain', 'sense', 'defined', 'below', 'as', 'a', 'consequence', 'we', 'infer', 'classical', 'result', 'of', 'serrin', 'of', 'existence', 'of', 'strong', 'solution', 'of', 'navierstok... | [-0.1544261477677755, 0.08910806042234033, -0.07915014065605339, 0.06549293675433687, -0.112007858428422, -0.150424850468432, -0.05151818998315385, 0.2671447682102591, -0.35398405740483546, -0.21712015096990156, 0.09447321602435206, -0.2563292093076546, -0.17544511457721532, 0.20293786211437742, -0.04680320939121269, 0... |
710.3402 | The 't Hooft Model As A Hologram | We consider the 3d dual of 1+1 dimensional large-N_c QCD with quarks in the
fundamental representation, also known as the 't Hooft model. 't Hooft solved
this model by deriving a Schroedinger equation for the wavefunction of a parton
inside the meson. In the scale-invariant limit, we show how this equation is
related... | hep-th hep-ph | we consider the 3d dual of 11 dimensional largen_c qcd with quarks in the fundamental representation also known as the t hooft model t hooft solved this model by deriving a schroedinger equation for the wavefunction of a parton inside the meson in the scaleinvariant limit we show how this equation is related by a trans... | [['we', 'consider', 'the', '3d', 'dual', 'of', '11', 'dimensional', 'largen_c', 'qcd', 'with', 'quarks', 'in', 'the', 'fundamental', 'representation', 'also', 'known', 'as', 'the', 't', 'hooft', 'model', 't', 'hooft', 'solved', 'this', 'model', 'by', 'deriving', 'a', 'schroedinger', 'equation', 'for', 'the', 'wavefunct... | [-0.07967894844523118, 0.12204636742151974, -0.09970912159702112, 0.07630117752863629, -0.0852376030064946, -0.11201776893332947, 0.011766297066793597, 0.31337654641143575, -0.23563269886744115, -0.21718240576586867, 0.0668241956484208, -0.2717840721842683, -0.13601665300598673, 0.09281321990036571, -0.0069971413625938... |
710.3403 | On the two-photon decay width of the sigma meson | We shortly report on the two-photon decay width of the light $\sigma$-meson
interpreted as a quarkonium state. Results are given in dependence on the
$\sigma$-mass and the constituent mass of the light quark. The triangle
quark-loop diagram, responsible for the two-photon transition, is carefully
evaluated: a term in... | hep-ph | we shortly report on the twophoton decay width of the light sigmameson interpreted as a quarkonium state results are given in dependence on the sigmamass and the constituent mass of the light quark the triangle quarkloop diagram responsible for the twophoton transition is carefully evaluated a term in the transition am... | [['we', 'shortly', 'report', 'on', 'the', 'twophoton', 'decay', 'width', 'of', 'the', 'light', 'sigmameson', 'interpreted', 'as', 'a', 'quarkonium', 'state', 'results', 'are', 'given', 'in', 'dependence', 'on', 'the', 'sigmamass', 'and', 'the', 'constituent', 'mass', 'of', 'the', 'light', 'quark', 'the', 'triangle', 'q... | [-0.10257745467658554, 0.21480909375739948, -0.07264839514967177, 0.12653922531907294, -0.017381207485284125, -0.0858229492269047, 0.07851325608994607, 0.36916728616579547, -0.19784067341914544, -0.268042068109735, 0.01946467763851755, -0.297822855443663, -0.07330564908928923, 0.16762254626623221, 0.03335152931797963, ... |
710.3404 | Coherent, multi-heterodyne spectroscopy using stabilized optical
frequency combs | The broadband, coherent nature of narrow-linewidth fiber frequency combs is
exploited to measure the full complex spectrum of a molecular gas through
multi-heterodyne spectroscopy. We measure the absorption and phase shift
experienced by each of 155,000 individual frequency comb lines, spaced by 100
MHz and spanning ... | physics.optics | the broadband coherent nature of narrowlinewidth fiber frequency combs is exploited to measure the full complex spectrum of a molecular gas through multiheterodyne spectroscopy we measure the absorption and phase shift experienced by each of 155000 individual frequency comb lines spaced by 100 mhz and spanning from 149... | [['the', 'broadband', 'coherent', 'nature', 'of', 'narrowlinewidth', 'fiber', 'frequency', 'combs', 'is', 'exploited', 'to', 'measure', 'the', 'full', 'complex', 'spectrum', 'of', 'a', 'molecular', 'gas', 'through', 'multiheterodyne', 'spectroscopy', 'we', 'measure', 'the', 'absorption', 'and', 'phase', 'shift', 'exper... | [-0.10577777714398957, 0.12638317305466223, -0.04377980901720537, -0.05141739149701022, -0.034538025314780486, -0.1255998350947496, 0.11637059327257776, 0.5228730640534697, -0.24185597074442897, -0.29596465267241, 0.06042405800765444, -0.24970508092778854, -0.04523259758863641, 0.232388474197052, 0.014511521268721628, ... |
710.3405 | Spectra of graph neighborhoods and scattering | Let $(G_\epsilon)_{\epsilon>0}$ be a family of '$\epsilon$-thin' Riemannian
manifolds modeled on a finite metric graph $G$, for example, the
$\epsilon$-neighborhood of an embedding of $G$ in some Euclidean space with
straight edges. We study the asymptotic behavior of the spectrum of the
Laplace-Beltrami operator on ... | math.SP math-ph math.AP math.MP | let g_epsilon_epsilon0 be a family of epsilonthin riemannian manifolds modeled on a finite metric graph g for example the epsilonneighborhood of an embedding of g in some euclidean space with straight edges we study the asymptotic behavior of the spectrum of the laplacebeltrami operator on g_epsilon as epsilonto 0 for ... | [['let', 'g_epsilon_epsilon0', 'be', 'a', 'family', 'of', 'epsilonthin', 'riemannian', 'manifolds', 'modeled', 'on', 'a', 'finite', 'metric', 'graph', 'g', 'for', 'example', 'the', 'epsilonneighborhood', 'of', 'an', 'embedding', 'of', 'g', 'in', 'some', 'euclidean', 'space', 'with', 'straight', 'edges', 'we', 'study', ... | [-0.12739164530257904, 0.047639938682224776, -0.10359191629382324, 0.05695287123020155, -0.09919872409629343, -0.07121844173395145, 0.018380125461549345, 0.363356061085169, -0.2571412243032411, -0.24357171200299219, 0.14743757944331684, -0.31566147743932793, -0.1349437825065523, 0.17979200842178691, -0.0796555093934398... |
710.3406 | Two-component jet simulations: I. Topological stability of analytical
MHD outflow solutions | Observations of collimated outflows in young stellar objects indicate that
several features of the jets can be understood by adopting the picture of a
two-component outflow, wherein a central stellar component around the jet axis
is surrounded by an extended disk-wind. The precise contribution of each
component may d... | astro-ph | observations of collimated outflows in young stellar objects indicate that several features of the jets can be understood by adopting the picture of a twocomponent outflow wherein a central stellar component around the jet axis is surrounded by an extended diskwind the precise contribution of each component may depend ... | [['observations', 'of', 'collimated', 'outflows', 'in', 'young', 'stellar', 'objects', 'indicate', 'that', 'several', 'features', 'of', 'the', 'jets', 'can', 'be', 'understood', 'by', 'adopting', 'the', 'picture', 'of', 'a', 'twocomponent', 'outflow', 'wherein', 'a', 'central', 'stellar', 'component', 'around', 'the', ... | [-0.12350604747259906, 0.08022279876030025, -0.1051693012663409, 0.07325554586266382, -0.06719281572682655, -0.08480105203150315, 0.003613162572733183, 0.3577171540310086, -0.2552703720015975, -0.2628750405557122, 0.13229909771157858, -0.24912492578721, -0.08128920564925683, 0.18344585931561094, 0.015263651563904211, 0... |
710.3407 | Little Higgs, Non-standard Higgs, No Higgs and All That | We give a brief review of recent developments in non-supersymmetric models
for electroweak symmetry breaking, including little Higgs, composite Higgs and
Higgsless theories. The new ideas such as extra dimensions, AdS/CFT
correspondence, dimension-deconstruction, and collective symmetry breaking
provide us new tools ... | hep-ph | we give a brief review of recent developments in nonsupersymmetric models for electroweak symmetry breaking including little higgs composite higgs and higgsless theories the new ideas such as extra dimensions adscft correspondence dimensiondeconstruction and collective symmetry breaking provide us new tools to construc... | [['we', 'give', 'a', 'brief', 'review', 'of', 'recent', 'developments', 'in', 'nonsupersymmetric', 'models', 'for', 'electroweak', 'symmetry', 'breaking', 'including', 'little', 'higgs', 'composite', 'higgs', 'and', 'higgsless', 'theories', 'the', 'new', 'ideas', 'such', 'as', 'extra', 'dimensions', 'adscft', 'correspo... | [-0.030848422012749618, 0.19851580165105603, -0.10107176851923183, 0.1884075069515887, -0.1936408684004919, -0.2660512940689795, -0.0006054949362651776, 0.32245196907197016, -0.217800154476979, -0.2925085458209959, 0.10521338174861493, -0.19858520464000876, -0.17087672859967007, 0.13550103020112395, -0.0762503757457233... |
710.3408 | Numerical solution of the radial Dirac equation in pseudopotential
construction | In the present work we study numerical solution of the radial Dirac equation
in a specific case - ab-initio pseudopotential generating process - which is
needed within the electronic structure calculations using a Density Functional
Theory (DFT) combined with a pseudopotential method. We give a brief
introduction to ... | physics.atom-ph | in the present work we study numerical solution of the radial dirac equation in a specific case abinitio pseudopotential generating process which is needed within the electronic structure calculations using a density functional theory dft combined with a pseudopotential method we give a brief introduction to dft derive... | [['in', 'the', 'present', 'work', 'we', 'study', 'numerical', 'solution', 'of', 'the', 'radial', 'dirac', 'equation', 'in', 'a', 'specific', 'case', 'abinitio', 'pseudopotential', 'generating', 'process', 'which', 'is', 'needed', 'within', 'the', 'electronic', 'structure', 'calculations', 'using', 'a', 'density', 'func... | [-0.08989546554765165, 0.02733220648848936, -0.12137396859870565, 0.08954678547302643, -0.06653786446861547, -0.10930114079059826, 0.060039949905588245, 0.35612990833216845, -0.24652902445417235, -0.28603358602038387, 0.041295909329853726, -0.3147984952524756, -0.16705384376374158, 0.1434831914939974, 0.048327608226864... |
710.3409 | Desingularizations of some Weighted Projective Planes | In this paper we discuss the desingularization algorithm for a toric surface.
In particular, we construct an iterable method of determining the
Hirzebruch-Jung continued fraction decomposition. These results are then
applied to weighted projective planes with at least one tivial weight,
${\mathbb P}(1,m,n)$. The pape... | math.AG | in this paper we discuss the desingularization algorithm for a toric surface in particular we construct an iterable method of determining the hirzebruchjung continued fraction decomposition these results are then applied to weighted projective planes with at least one tivial weight mathbb p1mn the paper concludes with ... | [['in', 'this', 'paper', 'we', 'discuss', 'the', 'desingularization', 'algorithm', 'for', 'a', 'toric', 'surface', 'in', 'particular', 'we', 'construct', 'an', 'iterable', 'method', 'of', 'determining', 'the', 'hirzebruchjung', 'continued', 'fraction', 'decomposition', 'these', 'results', 'are', 'then', 'applied', 'to'... | [-0.15262177101287402, 0.02205406998824369, -0.0884950862985039, -0.006869653489015866, -0.06700147069141008, -0.07270630890209424, 0.012814536972559597, 0.36422621226755153, -0.31327715671310824, -0.22226099985275874, 0.13104073789477216, -0.2483900849168238, -0.17550703994276232, 0.20983447121423587, -0.1195472986028... |
710.341 | Creation of neutral fundamental particles in the Weyl-Dirac version of
Wesson's IMT | Spherically symmetric entities filled with matter induced by the 5D Bulk may
be built in the empty 4D space-time. The substance of the entity, the latter
regarded as a fundamental particle, is characterized by the prematter equ. of
state P=-rho. the particle is coverede by a Schwarzschild-like envelope and
from the o... | gr-qc | spherically symmetric entities filled with matter induced by the 5d bulk may be built in the empty 4d spacetime the substance of the entity the latter regarded as a fundamental particle is characterized by the prematter equ of state prho the particle is coverede by a schwarzschildlike envelope and from the outside it i... | [['spherically', 'symmetric', 'entities', 'filled', 'with', 'matter', 'induced', 'by', 'the', '5d', 'bulk', 'may', 'be', 'built', 'in', 'the', 'empty', '4d', 'spacetime', 'the', 'substance', 'of', 'the', 'entity', 'the', 'latter', 'regarded', 'as', 'a', 'fundamental', 'particle', 'is', 'characterized', 'by', 'the', 'pr... | [-0.07975411678974827, 0.24593420707802663, -0.03975789508536116, 0.07376792282802748, -0.031105200598657335, -0.13923264455435605, -0.019492117233103377, 0.27357987734093064, -0.21305157218513818, -0.3000669179205922, 0.05448160203703647, -0.28588718961624576, -0.06291077608488843, 0.07735767314242649, -0.023668865121... |
710.3411 | Input Impedance, Nanocircuit Loading, and Radiation Tuning of Optical
Nanoantennas | Here we explore the radiation features of optical nanoantennas, analyzing the
concepts of input impedance, optical radiation resistance, impedance matching
and loading of plasmonic nanodipoles. We discuss how the concept of antenna
impedance may be applied to optical frequencies, and how its quantity may be
properly ... | cond-mat.mtrl-sci | here we explore the radiation features of optical nanoantennas analyzing the concepts of input impedance optical radiation resistance impedance matching and loading of plasmonic nanodipoles we discuss how the concept of antenna impedance may be applied to optical frequencies and how its quantity may be properly defined... | [['here', 'we', 'explore', 'the', 'radiation', 'features', 'of', 'optical', 'nanoantennas', 'analyzing', 'the', 'concepts', 'of', 'input', 'impedance', 'optical', 'radiation', 'resistance', 'impedance', 'matching', 'and', 'loading', 'of', 'plasmonic', 'nanodipoles', 'we', 'discuss', 'how', 'the', 'concept', 'of', 'ante... | [-0.13477065236549135, 0.13583474798288978, -0.05142472003713066, -0.03415388838721462, -0.11077032956858109, -0.15264981326267676, 0.03580966649180347, 0.5126408244494671, -0.27092761715391167, -0.2836888843549438, 0.05030455301788112, -0.23928866387103442, -0.21725674070141934, 0.20321116094580954, -0.079822289119302... |
710.3412 | Associated Production for the Standard Model Higgs at CDF | We report the latest result for the search for the standard model higgs
produced in association with a W and a Z boson at CDF. The results include
about 1 to 1.7 fb-1 of data collected by CDF in run II of the Tevatron. Novel
analysis techniques have been developed to enhance the sensitivity of these
searches.
| hep-ex | we report the latest result for the search for the standard model higgs produced in association with a w and a z boson at cdf the results include about 1 to 17 fb1 of data collected by cdf in run ii of the tevatron novel analysis techniques have been developed to enhance the sensitivity of these searches | [['we', 'report', 'the', 'latest', 'result', 'for', 'the', 'search', 'for', 'the', 'standard', 'model', 'higgs', 'produced', 'in', 'association', 'with', 'a', 'w', 'and', 'a', 'z', 'boson', 'at', 'cdf', 'the', 'results', 'include', 'about', '1', 'to', '17', 'fb1', 'of', 'data', 'collected', 'by', 'cdf', 'in', 'run', 'i... | [-0.0020354742086247392, 0.09154633347663962, -0.07872298197297935, 0.0706703473340001, -0.07923124745292098, -0.15224120521656515, 0.08336074035941508, 0.3333440112570922, -0.19557914790583023, -0.37802773223895775, 0.07788902449650331, -0.3376890329088558, 0.021668227748912677, 0.18171563127748014, 0.0740064206265583... |
710.3413 | Effective cone of $overline{M}_{0,n}$ for odd $n$ | In this work, we compute the effective cone of the space of $n$ pointed genus
0 rational curves, $\bar{M}_{0,n}$ for odd $n$. We will, in fact, use the
equivalence of $\bar{M}_{0,n}$ and the space of (semi) stable configurations of
$n$ weighted points on $\mathbb{CP}^{1}$ with special weight $(1,..., 1)$ up to
symmet... | math.AG | in this work we compute the effective cone of the space of n pointed genus 0 rational curves barm_0n for odd n we will in fact use the equivalence of barm_0n and the space of semi stable configurations of n weighted points on mathbbcp1 with special weight 1 1 up to symmetric group action | [['in', 'this', 'work', 'we', 'compute', 'the', 'effective', 'cone', 'of', 'the', 'space', 'of', 'n', 'pointed', 'genus', '0', 'rational', 'curves', 'barm_0n', 'for', 'odd', 'n', 'we', 'will', 'in', 'fact', 'use', 'the', 'equivalence', 'of', 'barm_0n', 'and', 'the', 'space', 'of', 'semi', 'stable', 'configurations', 'o... | [-0.20896081464296137, 0.14266100268879975, -0.08013793973993787, 0.05334201671346953, -0.04614427454631637, -0.1369545921959259, 0.060626760228640504, 0.3672075148809839, -0.27421187422307275, -0.23615260915485797, 0.06660105985227144, -0.2801332215442219, -0.15654486681213947, 0.15222017986148043, -0.0688155030107332... |
710.3414 | Kaon Weak Matrix Elements in 2+1 flavor DWF QCD | $K \to \pi$ and $K \to 0$ weak matrix elements of $\Delta S = 1$ operators
have been measured in 2+1 flavor domain wall fermion (DWF) QCD on (3 fm)$^3$
lattices with $a^{-1} = 1.73(3)$ GeV. As is well known, using these matrix
elements and chiral perturbation theory allows a determination of the $K \to
\pi \pi$ matri... | hep-lat | k to pi and k to 0 weak matrix elements of delta s 1 operators have been measured in 21 flavor domain wall fermion dwf qcd on 3 fm3 lattices with a1 1733 gev as is well known using these matrix elements and chiral perturbation theory allows a determination of the k to pi pi matrix elements that enter in the quantitativ... | [['k', 'to', 'pi', 'and', 'k', 'to', '0', 'weak', 'matrix', 'elements', 'of', 'delta', 's', '1', 'operators', 'have', 'been', 'measured', 'in', '21', 'flavor', 'domain', 'wall', 'fermion', 'dwf', 'qcd', 'on', '3', 'fm3', 'lattices', 'with', 'a1', '1733', 'gev', 'as', 'is', 'well', 'known', 'using', 'these', 'matrix', '... | [-0.08668755058242342, 0.2595290785049403, -0.050252810985602386, 0.05046637794881788, -0.028756718678609624, -0.10851294024375618, 0.1343073368046297, 0.39297919410330223, -0.16097466977596875, -0.2889871626524933, 0.04989341161420433, -0.3331219916377835, -0.018337830457071595, 0.09505645934467678, 0.0535917299296953... |
710.3415 | Modified gravity and the origin of inertia | Modified gravity theory is known to violate Birkhoff's theorem. We explore a
key consequence of this violation, the effect of distant matter in the Universe
on the motion of test particles. We find that when a particle is accelerated, a
force is experienced that is proportional to the particle's mass and
acceleration... | gr-qc astro-ph | modified gravity theory is known to violate birkhoffs theorem we explore a key consequence of this violation the effect of distant matter in the universe on the motion of test particles we find that when a particle is accelerated a force is experienced that is proportional to the particles mass and acceleration and act... | [['modified', 'gravity', 'theory', 'is', 'known', 'to', 'violate', 'birkhoffs', 'theorem', 'we', 'explore', 'a', 'key', 'consequence', 'of', 'this', 'violation', 'the', 'effect', 'of', 'distant', 'matter', 'in', 'the', 'universe', 'on', 'the', 'motion', 'of', 'test', 'particles', 'we', 'find', 'that', 'when', 'a', 'par... | [-0.12366908580380757, 0.18390916309519006, -0.15940739249137031, 0.08260169632142476, -0.10039424989996146, -0.1539001702123122, 0.001931517334014643, 0.29937104139077875, -0.24770370292078173, -0.3019725543272216, 0.01113448971903251, -0.2426795506783362, -0.1015530431593236, 0.2040804853199266, -0.06961868561172325,... |
710.3416 | A new level of photometric precision: WIRE observations of eclipsing
binary stars | The WIRE satellite was launched in March 1999 and was the first space mission
to do asteroseismology from space on a large number of stars. WIRE has produced
very high-precision photometry of a few hundred bright stars (V<6) with
temporal coverage of several weeks, including K giants, solar-like stars, delta
Scuti st... | astro-ph | the wire satellite was launched in march 1999 and was the first space mission to do asteroseismology from space on a large number of stars wire has produced very highprecision photometry of a few hundred bright stars v6 with temporal coverage of several weeks including k giants solarlike stars delta scuti stars and bet... | [['the', 'wire', 'satellite', 'was', 'launched', 'in', 'march', '1999', 'and', 'was', 'the', 'first', 'space', 'mission', 'to', 'do', 'asteroseismology', 'from', 'space', 'on', 'a', 'large', 'number', 'of', 'stars', 'wire', 'has', 'produced', 'very', 'highprecision', 'photometry', 'of', 'a', 'few', 'hundred', 'bright',... | [-0.11285071748138834, 0.1718184104603198, -0.060074079948078306, 0.02493754730537711, -0.14716097106048392, -0.0750110113793718, 0.10356202848451508, 0.3636698907699495, -0.15135935344640905, -0.3955435106782095, 0.07853314850667846, -0.3593572040258478, -0.09154285211647335, 0.28454137311985955, -0.13965701922729967,... |
710.3417 | Coupled-cluster single-double calculations of the relativistic energy
shifts in C IV, Na I, Mg II, Al III, Si IV, Ca II and Zn II | The relativistic coupled-cluster single-double method is used to calculate
the dependence of frequencies of strong $E1$-transitions in many monovalent
atoms and ions on the fine-structure constant $\alpha$. These transitions are
used in the search for manifestations of the variation of the fine-structure
constant in ... | physics.atom-ph | the relativistic coupledcluster singledouble method is used to calculate the dependence of frequencies of strong e1transitions in many monovalent atoms and ions on the finestructure constant alpha these transitions are used in the search for manifestations of the variation of the finestructure constant in quasar absorp... | [['the', 'relativistic', 'coupledcluster', 'singledouble', 'method', 'is', 'used', 'to', 'calculate', 'the', 'dependence', 'of', 'frequencies', 'of', 'strong', 'e1transitions', 'in', 'many', 'monovalent', 'atoms', 'and', 'ions', 'on', 'the', 'finestructure', 'constant', 'alpha', 'these', 'transitions', 'are', 'used', '... | [-0.08575303483972206, 0.09752793177481621, 0.006413737672471231, 0.08293792019004843, 0.016361522082720074, -0.12327998664770876, 0.010923040336027982, 0.45539976620385725, -0.1447695748309695, -0.3361500192043041, -0.03472673582784351, -0.33674625748948706, -0.04527367753607611, 0.2077896396006127, 0.0747599760971723... |
710.3418 | VHE gamma-rays from Westerlund 2 and implications for the inferred
energetics | The H.E.S.S. collaboration recently reported the discovery of VHE gamma-ray
emission coincident with the young stellar cluster Westerlund 2. This system is
known to host a population of hot, massive stars, and, most particularly, the
WR binary WR20a. Particle acceleration to TeV energies in Westerlund 2 can be
accomp... | astro-ph | the hess collaboration recently reported the discovery of vhe gammaray emission coincident with the young stellar cluster westerlund 2 this system is known to host a population of hot massive stars and most particularly the wr binary wr20a particle acceleration to tev energies in westerlund 2 can be accomplished in sev... | [['the', 'hess', 'collaboration', 'recently', 'reported', 'the', 'discovery', 'of', 'vhe', 'gammaray', 'emission', 'coincident', 'with', 'the', 'young', 'stellar', 'cluster', 'westerlund', '2', 'this', 'system', 'is', 'known', 'to', 'host', 'a', 'population', 'of', 'hot', 'massive', 'stars', 'and', 'most', 'particularl... | [-0.06483725758870065, 0.1893183022055883, -0.0029984560889610348, 0.17945877487595746, -0.09915598747792884, -0.07919040103645428, 0.04287698880458871, 0.40828804164261057, -0.18985447842388184, -0.37133613621573086, 0.03530799477880794, -0.29144244086468907, 0.05009372662955328, 0.21460013111219808, 0.037382204021897... |
710.3419 | Moderate deviations for Poisson--Dirichlet distribution | The Poisson--Dirichlet distribution arises in many different areas. The
parameter $\theta$ in the distribution is the scaled mutation rate of a
population in the context of population genetics. The limiting case of $\theta$
approaching infinity is practically motivated and has led to new, interesting
mathematical str... | math.PR | the poissondirichlet distribution arises in many different areas the parameter theta in the distribution is the scaled mutation rate of a population in the context of population genetics the limiting case of theta approaching infinity is practically motivated and has led to new interesting mathematical structures laws ... | [['the', 'poissondirichlet', 'distribution', 'arises', 'in', 'many', 'different', 'areas', 'the', 'parameter', 'theta', 'in', 'the', 'distribution', 'is', 'the', 'scaled', 'mutation', 'rate', 'of', 'a', 'population', 'in', 'the', 'context', 'of', 'population', 'genetics', 'the', 'limiting', 'case', 'of', 'theta', 'appr... | [-0.08503222391645847, 0.1078968636637969, -0.14341602957532776, 0.1205708206956018, -0.06128671179733259, -0.11526535163640225, 0.05282295524584893, 0.3112660897493684, -0.276271877110192, -0.28389106294234023, 0.08996634169150036, -0.25347995136951584, -0.13811228251111485, 0.20911019375855974, -0.08728084017073723, ... |
710.342 | Time Evolution of Disease Spread on Networks with Degree Heterogeneity | Two crucial elements facilitate the understanding and control of communicable
disease spread within a social setting. These components are, the underlying
contact structure among individuals that determines the pattern of disease
transmission; and the evolution of this pattern over time. Mathematical models
of infect... | q-bio.PE | two crucial elements facilitate the understanding and control of communicable disease spread within a social setting these components are the underlying contact structure among individuals that determines the pattern of disease transmission and the evolution of this pattern over time mathematical models of infectious d... | [['two', 'crucial', 'elements', 'facilitate', 'the', 'understanding', 'and', 'control', 'of', 'communicable', 'disease', 'spread', 'within', 'a', 'social', 'setting', 'these', 'components', 'are', 'the', 'underlying', 'contact', 'structure', 'among', 'individuals', 'that', 'determines', 'the', 'pattern', 'of', 'disease... | [-0.08609134072737236, 0.05683531995600788, -0.10970716772759001, 0.09806261772402129, -0.08380203384773008, -0.14910464665029263, 0.06934817450798748, 0.3912142142653465, -0.260359201097994, -0.2871161586034369, 0.10271529887125196, -0.25009005695911973, -0.24397025440183434, 0.18258321577533415, -0.06317232688161312,... |
710.3421 | Modular model building | Mathematical models are increasingly used in both academia and the
pharmaceutical industry to understand how phenotypes emerge from systems of
molecular interactions. However, their current construction as monolithic sets
of equations presents a fundamental barrier to progress. Overcoming this
requires modularity, en... | q-bio.MN | mathematical models are increasingly used in both academia and the pharmaceutical industry to understand how phenotypes emerge from systems of molecular interactions however their current construction as monolithic sets of equations presents a fundamental barrier to progress overcoming this requires modularity enabling... | [['mathematical', 'models', 'are', 'increasingly', 'used', 'in', 'both', 'academia', 'and', 'the', 'pharmaceutical', 'industry', 'to', 'understand', 'how', 'phenotypes', 'emerge', 'from', 'systems', 'of', 'molecular', 'interactions', 'however', 'their', 'current', 'construction', 'as', 'monolithic', 'sets', 'of', 'equa... | [-0.05695328721693451, 0.10977508782276085, -0.08841037587470575, 0.08152653419529088, -0.12910490226266638, -0.18953868728131057, 0.03951696472774659, 0.41981897046124295, -0.3192939210683107, -0.3647025430009567, 0.10404915594429309, -0.1743775859525028, -0.13037787014618515, 0.21820514198126537, -0.09288359958611961... |
710.3422 | A Simple Probabilistic Algorithm for Detecting Community Structure in
Social Networks | In this paper, we propose a novel semi-parametric probabilistic model which
considers interactions between different communities and can provide more
information about the network topology besides correctly detecting communities.
By using an additional parameter, our model can not only detect community
structure but ... | physics.soc-ph | in this paper we propose a novel semiparametric probabilistic model which considers interactions between different communities and can provide more information about the network topology besides correctly detecting communities by using an additional parameter our model can not only detect community structure but also d... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'novel', 'semiparametric', 'probabilistic', 'model', 'which', 'considers', 'interactions', 'between', 'different', 'communities', 'and', 'can', 'provide', 'more', 'information', 'about', 'the', 'network', 'topology', 'besides', 'correctly', 'detecting', 'communities', 'by'... | [-0.09965089794615822, 0.017698370179909013, -0.10052445448208489, 0.09626257863366999, -0.10863427714590566, -0.13363311486143384, 0.0734887426979952, 0.37791547264499836, -0.30304132042879084, -0.3558130476073957, 0.06189053085161351, -0.23954278517918415, -0.2541089392356934, 0.1404154120596597, -0.08205666270735393... |
710.3423 | Quasidiagonality of crossed products | We prove that the crossed product A x G of a separable, unital, quasidiagonal
C*- algebra A by a discrete, countable, amenable, maximally almost periodic
group G is quasidiagonal, provided that the action is almost periodic.
| math.OA | we prove that the crossed product a x g of a separable unital quasidiagonal c algebra a by a discrete countable amenable maximally almost periodic group g is quasidiagonal provided that the action is almost periodic | [['we', 'prove', 'that', 'the', 'crossed', 'product', 'a', 'x', 'g', 'of', 'a', 'separable', 'unital', 'quasidiagonal', 'c', 'algebra', 'a', 'by', 'a', 'discrete', 'countable', 'amenable', 'maximally', 'almost', 'periodic', 'group', 'g', 'is', 'quasidiagonal', 'provided', 'that', 'the', 'action', 'is', 'almost', 'perio... | [-0.24695830481747785, 0.2006835957419955, -0.11349741793755028, -0.001275546764696224, -0.10204375514553653, -0.16992438465563786, 0.03083257595749779, 0.49484699798954856, -0.3576075637506114, -0.04757413293959366, 0.1442508045454613, -0.2334664779353059, -0.10362242198445731, 0.18873679680756242, -0.1331053425868352... |
710.3424 | Growth, Structure and Properties of BiFeO3-BiCrO3 Films obtained by Dual
Cross Beam PLD | The properties of epitaxial Bi2FeCrO6 thin films, recently synthesized by
pulsed laser deposition, have partially confirmed the theoretical predictions
(i.e. a magnetic moment of 2 muB per formula unit and a polarization of ~80
microC/cm2 at 0K). The existence of magnetic ordering at room temperature for
this materia... | cond-mat.mtrl-sci | the properties of epitaxial bi2fecro6 thin films recently synthesized by pulsed laser deposition have partially confirmed the theoretical predictions ie a magnetic moment of 2 mub per formula unit and a polarization of 80 microccm2 at 0k the existence of magnetic ordering at room temperature for this material is an une... | [['the', 'properties', 'of', 'epitaxial', 'bi2fecro6', 'thin', 'films', 'recently', 'synthesized', 'by', 'pulsed', 'laser', 'deposition', 'have', 'partially', 'confirmed', 'the', 'theoretical', 'predictions', 'ie', 'a', 'magnetic', 'moment', 'of', '2', 'mub', 'per', 'formula', 'unit', 'and', 'a', 'polarization', 'of', ... | [-0.1275098956107806, 0.22754696148700504, -0.009732171353323394, -0.03046482606340357, -0.02300560123064736, -0.13074569454629772, 0.07946178469655164, 0.4730117900102441, -0.2871091220138678, -0.3255678130341555, 0.023905249581259874, -0.30547589605757547, -0.039603468324914945, 0.17891687798818842, 0.063661270360786... |
710.3425 | An entanglement measure for n-qubits | Recently, Coffman, Kundu, and Wootters introduced the residual entanglement
for three qubits to quantify the three-qubit entanglement in Phys. Rev. A 61,
052306 (2000). In Phys. Rev. A 65, 032304 (2007), we defined the residual
entanglement for $n$ qubits, whose values are between 0 and 1. In this paper,
we want to s... | quant-ph | recently coffman kundu and wootters introduced the residual entanglement for three qubits to quantify the threequbit entanglement in phys rev a 61 052306 2000 in phys rev a 65 032304 2007 we defined the residual entanglement for n qubits whose values are between 0 and 1 in this paper we want to show that the residual e... | [['recently', 'coffman', 'kundu', 'and', 'wootters', 'introduced', 'the', 'residual', 'entanglement', 'for', 'three', 'qubits', 'to', 'quantify', 'the', 'threequbit', 'entanglement', 'in', 'phys', 'rev', 'a', '61', '052306', '2000', 'in', 'phys', 'rev', 'a', '65', '032304', '2007', 'we', 'defined', 'the', 'residual', '... | [-0.14327853131107987, 0.2101376792731753, -0.010471644047647714, -0.013680830606608652, 0.0595634053577669, -0.2028365440480411, 0.04075347441365011, 0.3355167392455041, -0.17554209052585065, -0.2921676373295486, 0.017049801266985014, -0.3154045632481575, -0.1455844455747865, 0.1635678425896913, -0.12565147300250828, ... |
710.3426 | Some remarks on groupoids and small categories | This unpublished note contains some materials taken from my old study note on
groupoids and small categories. It contains a proof for the fact that any
groupoid is a group bundle over an equivalence relation. Moreover, the action
of a category $G$ on a category $H$ as well as the resulting semi-direct
product categor... | math.CT math.DS | this unpublished note contains some materials taken from my old study note on groupoids and small categories it contains a proof for the fact that any groupoid is a group bundle over an equivalence relation moreover the action of a category g on a category h as well as the resulting semidirect product category htimes_a... | [['this', 'unpublished', 'note', 'contains', 'some', 'materials', 'taken', 'from', 'my', 'old', 'study', 'note', 'on', 'groupoids', 'and', 'small', 'categories', 'it', 'contains', 'a', 'proof', 'for', 'the', 'fact', 'that', 'any', 'groupoid', 'is', 'a', 'group', 'bundle', 'over', 'an', 'equivalence', 'relation', 'moreo... | [-0.14370502382336023, 0.0897142469016349, -0.09783410807185382, 0.0744913614296255, -0.17566355099015443, -0.12814058080141533, 0.029117813024181618, 0.4218461685678334, -0.3177251927147719, -0.26600712818066474, 0.11388966598823776, -0.27712822449732644, -0.132019496344265, 0.1779558524665721, -0.2137956635086137, -0... |
710.3427 | Error Correction Capability of Column-Weight-Three LDPC Codes | In this paper, we investigate the error correction capability of
column-weight-three LDPC codes when decoded using the Gallager A algorithm. We
prove that the necessary condition for a code to correct $k \geq 5$ errors is
to avoid cycles of length up to $2k$ in its Tanner graph. As a consequence of
this result, we sh... | cs.IT math.IT | in this paper we investigate the error correction capability of columnweightthree ldpc codes when decoded using the gallager a algorithm we prove that the necessary condition for a code to correct k geq 5 errors is to avoid cycles of length up to 2k in its tanner graph as a consequence of this result we show that given... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'error', 'correction', 'capability', 'of', 'columnweightthree', 'ldpc', 'codes', 'when', 'decoded', 'using', 'the', 'gallager', 'a', 'algorithm', 'we', 'prove', 'that', 'the', 'necessary', 'condition', 'for', 'a', 'code', 'to', 'correct', 'k', 'geq', '5', 'errors', '... | [-0.19368628283532766, 0.08982762071600818, -0.0441784579767385, 0.10675130584302799, 0.024497583274381583, -0.22425431872789675, 0.09900331574333525, 0.38908416433976245, -0.2693972552008415, -0.308124053343148, 0.07610033868151911, -0.2585879162076738, -0.16209974699362006, 0.16607333470780689, -0.12473075685940765, ... |
710.3428 | Shell-shocked diffusion model for the light curve of SN2006gy | We explore a simple model for the high luminosity of SN 2006gy involving
photon diffusion of shock-deposited thermal energy. The distinguishing property
of the model is that the large ``stellar'' radius of 160 AU required to prevent
adiabatic losses is not the true stellar radius, but rather, the radius of an
opaque,... | astro-ph | we explore a simple model for the high luminosity of sn 2006gy involving photon diffusion of shockdeposited thermal energy the distinguishing property of the model is that the large stellar radius of 160 au required to prevent adiabatic losses is not the true stellar radius but rather the radius of an opaque unbound ci... | [['we', 'explore', 'a', 'simple', 'model', 'for', 'the', 'high', 'luminosity', 'of', 'sn', '2006gy', 'involving', 'photon', 'diffusion', 'of', 'shockdeposited', 'thermal', 'energy', 'the', 'distinguishing', 'property', 'of', 'the', 'model', 'is', 'that', 'the', 'large', 'stellar', 'radius', 'of', '160', 'au', 'required... | [-0.06395669352445024, 0.15022759089232246, -0.07929464290846154, 0.10832314042407422, -0.11087653070198468, -0.11148549632570035, 0.004771325442025371, 0.4049518946187192, -0.2504132601851783, -0.2925871980721613, 0.04001726357329385, -0.2769627824010127, -0.030617028583338358, 0.1593632874286834, -0.03185969490031025... |
710.3429 | Axion Inflation and Gravity Waves in String Theory | The majority of models of inflation in string theory predict an absence of
measurable gravitational waves, r << 10^{-3}. The most promising proposals for
making string theoretic models that yield measurable tensor fluctuations
involve axion fields with slightly broken shift symmetry. We consider such
models in detail... | hep-th astro-ph hep-ph | the majority of models of inflation in string theory predict an absence of measurable gravitational waves r 103 the most promising proposals for making string theoretic models that yield measurable tensor fluctuations involve axion fields with slightly broken shift symmetry we consider such models in detail with a part... | [['the', 'majority', 'of', 'models', 'of', 'inflation', 'in', 'string', 'theory', 'predict', 'an', 'absence', 'of', 'measurable', 'gravitational', 'waves', 'r', '103', 'the', 'most', 'promising', 'proposals', 'for', 'making', 'string', 'theoretic', 'models', 'that', 'yield', 'measurable', 'tensor', 'fluctuations', 'inv... | [-0.16807102668223836, 0.1826075937218515, -0.04975100811903498, 0.14609638651600107, -0.11416814706255017, -0.1988129346731252, -0.02356161289894122, 0.34710395508778413, -0.20258093286871112, -0.28384710930154794, 0.08428660357021726, -0.22120205526339953, -0.15788672238455287, 0.18970517644608792, -0.086174409726767... |
710.343 | Independent Signs of Lower Mass-Loss Rates for O-Type Stars | I discuss observational evidence -- independent of the direct spectral
diagnostics of stellar winds themselves -- suggesting that mass-loss rates for
O stars need to be revised downward by roughly a factor of three or more, in
line with recent observed mass-loss rates for clumped winds. These independent
constraints ... | astro-ph | i discuss observational evidence independent of the direct spectral diagnostics of stellar winds themselves suggesting that massloss rates for o stars need to be revised downward by roughly a factor of three or more in line with recent observed massloss rates for clumped winds these independent constraints include the ... | [['i', 'discuss', 'observational', 'evidence', 'independent', 'of', 'the', 'direct', 'spectral', 'diagnostics', 'of', 'stellar', 'winds', 'themselves', 'suggesting', 'that', 'massloss', 'rates', 'for', 'o', 'stars', 'need', 'to', 'be', 'revised', 'downward', 'by', 'roughly', 'a', 'factor', 'of', 'three', 'or', 'more', ... | [-0.04933967386085065, 0.19233391925375512, -0.04168237835550284, 0.1719541720912217, -0.13986737294954824, -0.10127361788057741, 0.12288166291298384, 0.44280354444809417, -0.1160049521924056, -0.32495273296978877, 0.06457984511259983, -0.23509420875083417, -0.0020164815780825598, 0.25686716981742413, -0.11586639766481... |
710.3431 | Possible Detection of a Pair Instability Supernova in the Modern
Universe, and Implications for the First Stars | SN 2006gy radiated far more energy in visual light than any other supernova
so far, and potential explanations for its energy demands have implications for
galactic chemical evolution and the deaths of the first stars. It remained
bright for over 200 days, longer than any normal supernova, and it radiated
more than 1... | astro-ph | sn 2006gy radiated far more energy in visual light than any other supernova so far and potential explanations for its energy demands have implications for galactic chemical evolution and the deaths of the first stars it remained bright for over 200 days longer than any normal supernova and it radiated more than 1e51 er... | [['sn', '2006gy', 'radiated', 'far', 'more', 'energy', 'in', 'visual', 'light', 'than', 'any', 'other', 'supernova', 'so', 'far', 'and', 'potential', 'explanations', 'for', 'its', 'energy', 'demands', 'have', 'implications', 'for', 'galactic', 'chemical', 'evolution', 'and', 'the', 'deaths', 'of', 'the', 'first', 'star... | [-0.05061628816810508, 0.1354761004248268, -0.04271539675447947, 0.15681991291001815, -0.14564622184843756, -0.15959445995171195, 0.06190675599366212, 0.42404374913670695, -0.2068125916637375, -0.29797060213548743, 0.057453903807282374, -0.30631911422376734, -0.02449685136021939, 0.2135111189388681, -0.0328028862960099... |
710.3432 | SU(5) grand unification on a domain-wall brane from an E_6-invariant
action | An SU(5) grand unification scheme for effective 3+1-dimensional fields
dynamically localised on a domain-wall brane is constructed. This is achieved
through the confluence of the clash-of-symmetries mechanism for symmetry
breaking through domain-wall formation, and the Dvali-Shifman gauge-boson
localisation idea. It ... | hep-ph hep-th | an su5 grand unification scheme for effective 31dimensional fields dynamically localised on a domainwall brane is constructed this is achieved through the confluence of the clashofsymmetries mechanism for symmetry breaking through domainwall formation and the dvalishifman gaugeboson localisation idea it requires an e_6... | [['an', 'su5', 'grand', 'unification', 'scheme', 'for', 'effective', '31dimensional', 'fields', 'dynamically', 'localised', 'on', 'a', 'domainwall', 'brane', 'is', 'constructed', 'this', 'is', 'achieved', 'through', 'the', 'confluence', 'of', 'the', 'clashofsymmetries', 'mechanism', 'for', 'symmetry', 'breaking', 'thro... | [-0.1911724176282039, 0.2346132841509655, -0.0653930022154463, 0.11737808563698132, -0.10563045724101558, -0.15963756322993763, 0.011850333932103807, 0.34391254108616864, -0.15830179476239659, -0.2750934703735175, 0.08090154782966438, -0.2431892079131847, -0.05906542485531468, 0.06579097714154171, -0.042180956655798796... |
710.3433 | Phase behavior and dynamics of a micelle-forming triblock copolymer
system | Synperonic F-108 (generic name, 'pluronic') is a micelle forming triblock
copolymer of type ABA, where A is polyethylene oxide (PEO) and B is
polypropylene oxide (PPO). At high temperatures, the hydrophobicity of the PPO
chains increase, and the pluronic molecules, when dissolved in an aqueous
medium, self-associate ... | cond-mat.soft cond-mat.mtrl-sci | synperonic f108 generic name pluronic is a micelle forming triblock copolymer of type aba where a is polyethylene oxide peo and b is polypropylene oxide ppo at high temperatures the hydrophobicity of the ppo chains increase and the pluronic molecules when dissolved in an aqueous medium selfassociate into spherical mice... | [['synperonic', 'f108', 'generic', 'name', 'pluronic', 'is', 'a', 'micelle', 'forming', 'triblock', 'copolymer', 'of', 'type', 'aba', 'where', 'a', 'is', 'polyethylene', 'oxide', 'peo', 'and', 'b', 'is', 'polypropylene', 'oxide', 'ppo', 'at', 'high', 'temperatures', 'the', 'hydrophobicity', 'of', 'the', 'ppo', 'chains'... | [-0.1259287166170629, 0.24404319568734736, -0.06737079671377619, -0.022852099246547325, 0.00016927191634373418, -0.129754929934064, 0.03884491214317641, 0.4186313995825393, -0.29809919411197233, -0.2533081010479498, 0.08536014292478616, -0.284580936210386, -0.11209025189482373, 0.12755028488288814, 0.00890404368685375,... |
710.3434 | Decay properties of charm and beauty open flavour mesons | The masses of $S$ and $P$ states, pseudoscalar and vector decay constants,
leptonic, semileptonic decay widths of charm (D) and beauty (B) open flavour
mesons have been computed in the framework of Coulomb and power potential of
the form $V(r)=-\frac{\alpha_c}{r}+A r^{\nu}$. The results are compared with
other theore... | hep-ph | the masses of s and p states pseudoscalar and vector decay constants leptonic semileptonic decay widths of charm d and beauty b open flavour mesons have been computed in the framework of coulomb and power potential of the form vrfracalpha_cra rnu the results are compared with other theoretical as well as experimental r... | [['the', 'masses', 'of', 's', 'and', 'p', 'states', 'pseudoscalar', 'and', 'vector', 'decay', 'constants', 'leptonic', 'semileptonic', 'decay', 'widths', 'of', 'charm', 'd', 'and', 'beauty', 'b', 'open', 'flavour', 'mesons', 'have', 'been', 'computed', 'in', 'the', 'framework', 'of', 'coulomb', 'and', 'power', 'potenti... | [-0.030382179593632243, 0.2491784635579811, -0.018475187257072836, 0.10712960130482349, -0.02308908930786376, -0.20695996804619735, 0.07038920450041879, 0.3384124800422282, -0.21334027987465543, -0.23454039533323837, -0.02965364561477711, -0.3562154892726608, 0.0230619457005611, 0.139484300392346, 0.13186930332614002, ... |
710.3435 | Numerical experimentation within GRworkbench | The software tool GRworkbench is an ongoing project in visual, numerical
General Relativity at The Australian National University. This year,
GRworkbench has been significantly extended to facilitate numerical
experimentation. The numerical differential geometric engine has been rewritten
using functional programming... | gr-qc | the software tool grworkbench is an ongoing project in visual numerical general relativity at the australian national university this year grworkbench has been significantly extended to facilitate numerical experimentation the numerical differential geometric engine has been rewritten using functional programming techn... | [['the', 'software', 'tool', 'grworkbench', 'is', 'an', 'ongoing', 'project', 'in', 'visual', 'numerical', 'general', 'relativity', 'at', 'the', 'australian', 'national', 'university', 'this', 'year', 'grworkbench', 'has', 'been', 'significantly', 'extended', 'to', 'facilitate', 'numerical', 'experimentation', 'the', '... | [-0.06157149723080616, 0.0005458936288883888, -0.15018959734953066, 0.08099177903261598, -0.11276682901102529, -0.11732032956222499, -0.006623162002193445, 0.35471147831591815, -0.2168425169407407, -0.34146384290268633, 0.14069703627278893, -0.2296441641828701, -0.13308766023346935, 0.26229964841843983, -0.069636570690... |
710.3436 | Spontaneous Emergence of Modularity in a Model of Evolving Individuals | We investigate the selective forces that promote the emergence of modularity
in nature. We demonstrate the spontaneous emergence of modularity in a
population of individuals that evolve in a changing environment. We show that
the level of modularity correlates with the rapidity and severity of
environmental change. T... | q-bio.PE | we investigate the selective forces that promote the emergence of modularity in nature we demonstrate the spontaneous emergence of modularity in a population of individuals that evolve in a changing environment we show that the level of modularity correlates with the rapidity and severity of environmental change the mo... | [['we', 'investigate', 'the', 'selective', 'forces', 'that', 'promote', 'the', 'emergence', 'of', 'modularity', 'in', 'nature', 'we', 'demonstrate', 'the', 'spontaneous', 'emergence', 'of', 'modularity', 'in', 'a', 'population', 'of', 'individuals', 'that', 'evolve', 'in', 'a', 'changing', 'environment', 'we', 'show', ... | [-0.16583423299704908, 0.1616690204458772, -0.09393552481447176, 0.09839462133009307, -0.020839494773216786, -0.044620008323021154, 0.04823146015405655, 0.37683435553504574, -0.2991056093665701, -0.3041695722889516, 0.042365153997345396, -0.21500769531935132, -0.24197319113919813, 0.08056165650486946, -0.06897026678467... |
710.3437 | Electronic Structures of CaAlSi with Different Stacking AlSi Layers by
First-Principles Calculations | The full-potential linear augmented plane-wave calculations have been applied
to investigate the systematic change of electronic structures in CaAlSi due to
different stacking sequences of AlSi layers. The present ab-initio calculations
have revealed that the multistacking, buckling and 60 degrees rotation of AlSi
la... | cond-mat.supr-con | the fullpotential linear augmented planewave calculations have been applied to investigate the systematic change of electronic structures in caalsi due to different stacking sequences of alsi layers the present abinitio calculations have revealed that the multistacking buckling and 60 degrees rotation of alsi layer aff... | [['the', 'fullpotential', 'linear', 'augmented', 'planewave', 'calculations', 'have', 'been', 'applied', 'to', 'investigate', 'the', 'systematic', 'change', 'of', 'electronic', 'structures', 'in', 'caalsi', 'due', 'to', 'different', 'stacking', 'sequences', 'of', 'alsi', 'layers', 'the', 'present', 'abinitio', 'calcula... | [-0.16739175924377112, 0.09238338216032269, -0.06120223337289902, 0.0006714686813179107, -0.04692733357866517, -0.07054718886708132, 0.09062348622457841, 0.41263968641746096, -0.286502181016634, -0.32381292521557975, -0.004709180929714534, -0.30070228657512144, -0.18209142363073913, 0.14076246452657917, 0.0490123343785... |
710.3438 | Can one detect passage of small black hole through the Earth? | The energy losses of a small black hole passing through the Earth are
examined. In particular, we investigate the excitations in the frequency range
accessible to modern acoustic detectors. The main contribution to the effect is
given by the coherent sound radiation of the Cherenkov type.
| astro-ph gr-qc physics.geo-ph | the energy losses of a small black hole passing through the earth are examined in particular we investigate the excitations in the frequency range accessible to modern acoustic detectors the main contribution to the effect is given by the coherent sound radiation of the cherenkov type | [['the', 'energy', 'losses', 'of', 'a', 'small', 'black', 'hole', 'passing', 'through', 'the', 'earth', 'are', 'examined', 'in', 'particular', 'we', 'investigate', 'the', 'excitations', 'in', 'the', 'frequency', 'range', 'accessible', 'to', 'modern', 'acoustic', 'detectors', 'the', 'main', 'contribution', 'to', 'the', ... | [-0.15744212247512263, 0.211241462369166, -0.008461350767427812, 0.12594616199772724, -0.08036867948248982, -0.013886683569897128, 0.010670993993382739, 0.3342924765513643, -0.26473176147302857, -0.291415530823819, 0.0747993439031036, -0.3336423482219486, -0.06421969607269959, 0.2478955980066372, -0.01692012793627446, ... |
710.3439 | Utility-Based Wireless Resource Allocation for Variable Rate
Transmission | For most wireless services with variable rate transmission, both average rate
and rate oscillation are important performance metrics. The traditional
performance criterion, utility of average transmission rate, boosts the average
rate but also results in high rate oscillations. We introduce a utility
function of inst... | cs.NI | for most wireless services with variable rate transmission both average rate and rate oscillation are important performance metrics the traditional performance criterion utility of average transmission rate boosts the average rate but also results in high rate oscillations we introduce a utility function of instantaneo... | [['for', 'most', 'wireless', 'services', 'with', 'variable', 'rate', 'transmission', 'both', 'average', 'rate', 'and', 'rate', 'oscillation', 'are', 'important', 'performance', 'metrics', 'the', 'traditional', 'performance', 'criterion', 'utility', 'of', 'average', 'transmission', 'rate', 'boosts', 'the', 'average', 'r... | [-0.22235802579772376, 0.029587075641598938, -0.017149318670988945, 0.026120102378890675, -0.04420496417088029, -0.1982562039486146, 0.14132196828722954, 0.41549391887974046, -0.2925802005186636, -0.27707798264758743, 0.13083017890618276, -0.22456054661112526, -0.1277054741276779, 0.2566842611582167, -0.087734865677623... |
710.344 | Five-dimensional Superfield Supergravity | We present a projective superspace formulation for matter-coupled simple
supergravity in five dimensions. Our starting point is the superspace
realization for the minimal supergravity multiplet proposed by Howe in 1981. We
introduce various off-shell supermultiplets (i.e. hypermultiplets, tensor and
vector multiplets... | hep-th | we present a projective superspace formulation for mattercoupled simple supergravity in five dimensions our starting point is the superspace realization for the minimal supergravity multiplet proposed by howe in 1981 we introduce various offshell supermultiplets ie hypermultiplets tensor and vector multiplets that desc... | [['we', 'present', 'a', 'projective', 'superspace', 'formulation', 'for', 'mattercoupled', 'simple', 'supergravity', 'in', 'five', 'dimensions', 'our', 'starting', 'point', 'is', 'the', 'superspace', 'realization', 'for', 'the', 'minimal', 'supergravity', 'multiplet', 'proposed', 'by', 'howe', 'in', '1981', 'we', 'intr... | [-0.12019719915343044, 0.15547732741612455, 0.020716452606670235, 0.07210040286198542, -0.1168157324174662, -0.23058560537807035, -0.11174604605691021, 0.3293403268528535, -0.07663291690709151, -0.26400313923216384, 0.0893489780554892, -0.2693844871499333, -0.2486920280220068, 0.06542762273760594, -0.10246634112706449,... |
710.3441 | Electron - nuclear recoil discrimination by pulse shape analysis | In the framework of the ``ULTIMA'' project, we use ultra cold superfluid 3He
bolometers for the direct detection of single particle events, aimed for a
future use as a dark matter detector. One parameter of the pulse shape observed
after such an event is the thermalization time constant. Until now it was
believed tha... | physics.ins-det | in the framework of the ultima project we use ultra cold superfluid 3he bolometers for the direct detection of single particle events aimed for a future use as a dark matter detector one parameter of the pulse shape observed after such an event is the thermalization time constant until now it was believed that this par... | [['in', 'the', 'framework', 'of', 'the', 'ultima', 'project', 'we', 'use', 'ultra', 'cold', 'superfluid', '3he', 'bolometers', 'for', 'the', 'direct', 'detection', 'of', 'single', 'particle', 'events', 'aimed', 'for', 'a', 'future', 'use', 'as', 'a', 'dark', 'matter', 'detector', 'one', 'parameter', 'of', 'the', 'pulse... | [-0.08678426327230024, 0.2142324798697392, -0.1159587804120311, 0.09518076745265987, -0.057192573689447704, -0.08518155072315418, 0.026264491714229267, 0.3544328130304444, -0.2124536037791428, -0.3394838343335947, 0.07505608525623621, -0.30783021102336133, -0.07260823421890286, 0.2205232502286484, 0.009887724772311193,... |
710.3442 | Measuring overlaps in mesoscopic spin glasses via conductance
fluctuations | We consider the electonic transport in a mesoscopic metallic spin glasses. We
show that the distribution of overlaps between spin configurations can be
inferred from the reduction of the conductance fluctuations by the magnetic
impurities. Using this property, we propose new experimental protocols to probe
spin glass... | cond-mat.dis-nn | we consider the electonic transport in a mesoscopic metallic spin glasses we show that the distribution of overlaps between spin configurations can be inferred from the reduction of the conductance fluctuations by the magnetic impurities using this property we propose new experimental protocols to probe spin glasses di... | [['we', 'consider', 'the', 'electonic', 'transport', 'in', 'a', 'mesoscopic', 'metallic', 'spin', 'glasses', 'we', 'show', 'that', 'the', 'distribution', 'of', 'overlaps', 'between', 'spin', 'configurations', 'can', 'be', 'inferred', 'from', 'the', 'reduction', 'of', 'the', 'conductance', 'fluctuations', 'by', 'the', '... | [-0.16058135558851064, 0.24809326520189642, -0.10245877479668707, 0.05808086515171453, 0.009780023922212422, -0.08414951815269887, 0.03531651973724365, 0.39774822928011416, -0.30612030405551194, -0.2889078129082918, 0.00657138237496838, -0.2944552992656827, -0.14799196790903807, 0.1504139931872487, 0.019972366057336332... |
710.3443 | DPA on quasi delay insensitive asynchronous circuits: formalization and
improvement | The purpose of this paper is to formally specify a flow devoted to the design
of Differential Power Analysis (DPA) resistant QDI asynchronous circuits. The
paper first proposes a formal modeling of the electrical signature of QDI
asynchronous circuits. The DPA is then applied to the formal model in order to
identify ... | cs.AR | the purpose of this paper is to formally specify a flow devoted to the design of differential power analysis dpa resistant qdi asynchronous circuits the paper first proposes a formal modeling of the electrical signature of qdi asynchronous circuits the dpa is then applied to the formal model in order to identify the so... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'formally', 'specify', 'a', 'flow', 'devoted', 'to', 'the', 'design', 'of', 'differential', 'power', 'analysis', 'dpa', 'resistant', 'qdi', 'asynchronous', 'circuits', 'the', 'paper', 'first', 'proposes', 'a', 'formal', 'modeling', 'of', 'the', 'electrical', 'signa... | [-0.15689968385765057, -0.027410290746660536, -0.0776884892767065, 0.02081992396341867, -0.06479735372148537, -0.12842131209863203, 0.04843741854433012, 0.3201152195923784, -0.3005155852755134, -0.2841714335228787, 0.08769775948387812, -0.25436921936742374, -0.15849047096634514, 0.1870093873644436, -0.12525132874267572... |
710.3444 | Strangeness Content of the Nucleon in the \chiCQM_{config} | Several parameters characterizing the strangeness content of the nucleon have
been calculated in the chiral constituent quark model with configuration mixing
(\chiCQM_{config}) which is known to provide a satisfactory explanation of the
``proton spin problem'' and related issues. In particular, we have calculated
the... | hep-ph | several parameters characterizing the strangeness content of the nucleon have been calculated in the chiral constituent quark model with configuration mixing chicqm_config which is known to provide a satisfactory explanation of the proton spin problem and related issues in particular we have calculated the strange spin... | [['several', 'parameters', 'characterizing', 'the', 'strangeness', 'content', 'of', 'the', 'nucleon', 'have', 'been', 'calculated', 'in', 'the', 'chiral', 'constituent', 'quark', 'model', 'with', 'configuration', 'mixing', 'chicqm_config', 'which', 'is', 'known', 'to', 'provide', 'a', 'satisfactory', 'explanation', 'of... | [-0.11321736896631888, 0.2748273716695459, -0.03863569918448235, 0.1153003961495631, -0.03886849541991654, -0.09980772855855284, 0.06407723005280119, 0.31809916627584117, -0.1611514921244787, -0.24163688393770763, -0.05830202563227809, -0.340836813046348, -0.010034167825585544, 0.04629236472872003, 0.06735540528108577,... |
710.3445 | Vacuum densities for a thick brane in AdS spacetime | For a massive scalar field with general curvature coupling parameter we
evaluate Wightman function, vacuum expectation values of the field square and
the energy-momentum tensor induced by a $Z_{2}$-symmetric brane with finite
thickness located on $(D+1)$-dimensional AdS bulk. For the general case of
static plane symm... | hep-th | for a massive scalar field with general curvature coupling parameter we evaluate wightman function vacuum expectation values of the field square and the energymomentum tensor induced by a z_2symmetric brane with finite thickness located on d1dimensional ads bulk for the general case of static plane symmetric interior s... | [['for', 'a', 'massive', 'scalar', 'field', 'with', 'general', 'curvature', 'coupling', 'parameter', 'we', 'evaluate', 'wightman', 'function', 'vacuum', 'expectation', 'values', 'of', 'the', 'field', 'square', 'and', 'the', 'energymomentum', 'tensor', 'induced', 'by', 'a', 'z_2symmetric', 'brane', 'with', 'finite', 'th... | [-0.1661942844910204, 0.1938365478222534, -0.016872792335619266, 0.07704081713148442, -0.12132904640349902, -0.10612794836051762, -0.08007735595793317, 0.30566797545179725, -0.16587728022928594, -0.2132492651035519, 0.07478732569572075, -0.276673850751678, -0.09992754466611108, 0.11453941008321157, -0.00772131168127280... |
710.3446 | Conformal Invariance for Certain Models of the Bond-Triangular Type | Following the approach outlined in [18], convergence to SLE6 of the
Exploration Processes for the correlated bond-triangular type models studied in
[7] is established. This puts the said models in the same universality class as
the standard site percolation model on the triangular lattice [19]. The result
is proven f... | math-ph math.MP math.PR | following the approach outlined in 18 convergence to sle6 of the exploration processes for the correlated bondtriangular type models studied in 7 is established this puts the said models in the same universality class as the standard site percolation model on the triangular lattice 19 the result is proven for all domai... | [['following', 'the', 'approach', 'outlined', 'in', '18', 'convergence', 'to', 'sle6', 'of', 'the', 'exploration', 'processes', 'for', 'the', 'correlated', 'bondtriangular', 'type', 'models', 'studied', 'in', '7', 'is', 'established', 'this', 'puts', 'the', 'said', 'models', 'in', 'the', 'same', 'universality', 'class'... | [-0.07634049952806284, 0.1137747329914765, -0.04670908404763655, 0.1239583756278513, -0.00022501740161152113, -0.1742026901005634, 0.0386234889599672, 0.30763138545721413, -0.21913839665995466, -0.24571321818179317, 0.13523993240059576, -0.24398470011406712, -0.12630978262140638, 0.213136716166489, -0.04803616057393983... |
710.3447 | Problems of Testology | Some problems of testology are discussed.
| stat.AP | some problems of testology are discussed | [['some', 'problems', 'of', 'testology', 'are', 'discussed']] | [-0.1900975201278925, 0.13659498170018197, 0.0812535636126995, 0.22356674075126648, -0.08320086598396301, -0.1807027354836464, -0.15450496412813663, 0.4628769338130951, -0.29639066085219384, -0.20993409901857377, 0.3633113205432892, -0.3283703548833728, -0.19256386533379555, 0.41901132464408875, -0.14266763292253018, 0... |
710.3448 | Spin Vortex in Magnon BEC of Superfluid 3He-B | The phenomenon of the spontaneous phase-coherent precession of magnetization
in superfluid 3He and the related effects of spin superfluidity are based on
the true Bose-Einstein condensation of magnons. Several different magnon BEC
states have been observed: homogeneously precessing domain (HPD); BEC
condensation in t... | cond-mat.other | the phenomenon of the spontaneous phasecoherent precession of magnetization in superfluid 3he and the related effects of spin superfluidity are based on the true boseeinstein condensation of magnons several different magnon bec states have been observed homogeneously precessing domain hpd bec condensation in the spinor... | [['the', 'phenomenon', 'of', 'the', 'spontaneous', 'phasecoherent', 'precession', 'of', 'magnetization', 'in', 'superfluid', '3he', 'and', 'the', 'related', 'effects', 'of', 'spin', 'superfluidity', 'are', 'based', 'on', 'the', 'true', 'boseeinstein', 'condensation', 'of', 'magnons', 'several', 'different', 'magnon', '... | [-0.25967898937049266, 0.37982791675062016, -0.06275040527067051, 0.07286893512020637, -0.06538341824907339, -0.13369917760378328, -0.0017687282685575813, 0.36671585804279677, -0.2221994593782329, -0.2013419794732298, -0.016378455248061866, -0.2795175594202746, -0.005460591387303396, 0.2092627788915288, 0.0942453385983... |
710.3449 | New non-abelian effects on D branes | We extend the Myers dielectric effect to configurations with angular
momentum. The resulting time-dependent N D0 brane bound states can be
interpreted as describing rotating fuzzy ellipsoids. A similar solution exists
also in the presence of a RR magnetic field, that we study in detail. We show
that, for any finite N... | hep-th | we extend the myers dielectric effect to configurations with angular momentum the resulting timedependent n d0 brane bound states can be interpreted as describing rotating fuzzy ellipsoids a similar solution exists also in the presence of a rr magnetic field that we study in detail we show that for any finite n above a... | [['we', 'extend', 'the', 'myers', 'dielectric', 'effect', 'to', 'configurations', 'with', 'angular', 'momentum', 'the', 'resulting', 'timedependent', 'n', 'd0', 'brane', 'bound', 'states', 'can', 'be', 'interpreted', 'as', 'describing', 'rotating', 'fuzzy', 'ellipsoids', 'a', 'similar', 'solution', 'exists', 'also', 'i... | [-0.17422314192573476, 0.18852818724533865, -0.06916475903612804, 0.08393973135070441, -0.040326765725669796, -0.14039124844098233, 0.017271511396034365, 0.3280470310008689, -0.1908079021999434, -0.28163750995786174, 0.022935609802865256, -0.25310277942032233, -0.11347613053728048, 0.10945983320053616, 0.00452959564297... |
710.345 | Spin up and phase fluctuations in the timing of the accreting
millisecond pulsar XTE J1807-294 | We performed a timing analysis of the 2003 outburst of the accreting X-ray
millisecond pulsar XTE J1807-294 observed by RXTE. Using recently refined
orbital parameters we report for the first time a precise estimate of the spin
frequency and of the spin frequency derivative. The phase delays of the pulse
profile show... | astro-ph | we performed a timing analysis of the 2003 outburst of the accreting xray millisecond pulsar xte j1807294 observed by rxte using recently refined orbital parameters we report for the first time a precise estimate of the spin frequency and of the spin frequency derivative the phase delays of the pulse profile show a str... | [['we', 'performed', 'a', 'timing', 'analysis', 'of', 'the', '2003', 'outburst', 'of', 'the', 'accreting', 'xray', 'millisecond', 'pulsar', 'xte', 'j1807294', 'observed', 'by', 'rxte', 'using', 'recently', 'refined', 'orbital', 'parameters', 'we', 'report', 'for', 'the', 'first', 'time', 'a', 'precise', 'estimate', 'of... | [-0.17921401333088788, 0.15156592405193287, -0.07671677217097438, 0.06904044358452666, -0.07066208753219273, -0.08460610794177878, 0.09041123035629946, 0.40494073100437944, -0.2353487855506111, -0.29209289581714465, 0.12069824404846129, -0.2622724156483725, -0.06795247066604913, 0.24413297121645883, -0.0324439103569602... |
710.3451 | Comlexity of prime-dimensional sequences over a finite field | V.I. Arnold has recently defined the complexity of a sequence of $n$ zeros
and ones with the help of the operator of finite differences. In this paper we
describe the results obtained for almost most complicated sequences of elements
of a finite field, whose dimension $n$ is a prime number. We prove that with
$n\to \... | math.NT math.DS math.RT | vi arnold has recently defined the complexity of a sequence of n zeros and ones with the help of the operator of finite differences in this paper we describe the results obtained for almost most complicated sequences of elements of a finite field whose dimension n is a prime number we prove that with nto infty this pro... | [['vi', 'arnold', 'has', 'recently', 'defined', 'the', 'complexity', 'of', 'a', 'sequence', 'of', 'n', 'zeros', 'and', 'ones', 'with', 'the', 'help', 'of', 'the', 'operator', 'of', 'finite', 'differences', 'in', 'this', 'paper', 'we', 'describe', 'the', 'results', 'obtained', 'for', 'almost', 'most', 'complicated', 'se... | [-0.1740362227224467, 0.1192525705943505, -0.09414146935338513, 0.06960567482338663, -0.03460895634877185, -0.11451280364570648, 0.008453921766455383, 0.32887256585813146, -0.2847404897970192, -0.25986144671894673, 0.05466048529151043, -0.2708662478049008, -0.17325327605858706, 0.18990796310990526, -0.04658938952509248... |
710.3452 | On Bost-Connes type systems for number fields | We give a complete description of the phase transition of the Bost-Connes
type systems for number fields recently introduced by
Connes-Marcolli-Ramachandran and Ha-Paugam. We also introduce a notion of
K-lattices and discuss an interpretation of these systems in terms of
1-dimensional K-lattices.
| math.OA math.NT | we give a complete description of the phase transition of the bostconnes type systems for number fields recently introduced by connesmarcolliramachandran and hapaugam we also introduce a notion of klattices and discuss an interpretation of these systems in terms of 1dimensional klattices | [['we', 'give', 'a', 'complete', 'description', 'of', 'the', 'phase', 'transition', 'of', 'the', 'bostconnes', 'type', 'systems', 'for', 'number', 'fields', 'recently', 'introduced', 'by', 'connesmarcolliramachandran', 'and', 'hapaugam', 'we', 'also', 'introduce', 'a', 'notion', 'of', 'klattices', 'and', 'discuss', 'an... | [-0.1730170935159549, 0.1101011310620379, -0.05197861529886723, 0.03531483341939747, -0.01689191102050245, -0.06358827538788318, 0.04226864012889564, 0.28105340329930184, -0.2325878491741605, -0.2799604287371039, 0.08344935680215712, -0.1980842475546524, -0.22715132373850794, 0.1972227635793388, -0.10317308059893548, 0... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.