id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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707.413 | Study of the process e+e- -> omega p0 with the KLOE detector | Using ~600 pb-1 collected with the KLOE detector at DAPhiNE, we have studied
the production cross section of pi+ pi- pi0 pi0 and p0p0 gamma final states in
e+e- collisions at center of mass energies between 1000 and 1030 MeV. By
fitting the observed interference pattern around Mphi for both final states, we
extract a... | hep-ex | using 600 pb1 collected with the kloe detector at daphine we have studied the production cross section of pi pi pi0 pi0 and p0p0 gamma final states in ee collisions at center of mass energies between 1000 and 1030 mev by fitting the observed interference pattern around mphi for both final states we extract a measuremen... | [['using', '600', 'pb1', 'collected', 'with', 'the', 'kloe', 'detector', 'at', 'daphine', 'we', 'have', 'studied', 'the', 'production', 'cross', 'section', 'of', 'pi', 'pi', 'pi0', 'pi0', 'and', 'p0p0', 'gamma', 'final', 'states', 'in', 'ee', 'collisions', 'at', 'center', 'of', 'mass', 'energies', 'between', '1000', 'a... | [-0.1028443339696811, 0.2738830819798186, -0.10129023165926662, 0.0807123949765697, 0.003242589198296543, -0.12698212648965707, 0.1453588788953516, 0.26132987845371397, -0.16808622802766546, -0.2501952658076193, -0.13240221590110526, -0.4601615625180939, 0.11927921336880604, 0.12934317660803163, 0.16890086956834782, 0.... |
707.4131 | Formation of MnI lines in the solar atmosphere | We present a detailed NLTE analysis of 39 MnI lines in the solar spectrum.
The influence of NLTE effects on the line formation and element abundance is
investigated. Our goal is the derivation of solar log gfe values for manganese
lines, which will later be used in differential abundance analysis of
metal-poor stars.... | astro-ph | we present a detailed nlte analysis of 39 mni lines in the solar spectrum the influence of nlte effects on the line formation and element abundance is investigated our goal is the derivation of solar log gfe values for manganese lines which will later be used in differential abundance analysis of metalpoor stars the me... | [['we', 'present', 'a', 'detailed', 'nlte', 'analysis', 'of', '39', 'mni', 'lines', 'in', 'the', 'solar', 'spectrum', 'the', 'influence', 'of', 'nlte', 'effects', 'on', 'the', 'line', 'formation', 'and', 'element', 'abundance', 'is', 'investigated', 'our', 'goal', 'is', 'the', 'derivation', 'of', 'solar', 'log', 'gfe',... | [-0.026397565254868742, 0.07489207056585137, -0.007197809470661359, 0.07944667440846916, 0.009562774874171107, -0.10244370625723757, 0.04159074775710723, 0.40649101652390995, -0.13846409877543675, -0.34403685174424553, -0.0091393976160143, -0.31580023151723535, -0.03887684135463651, 0.15410317433737844, 0.0038826904837... |
707.4132 | Comment on "On an identity for the volume integral of the square of a
vector field" | Stewart has provided a position-space derivation of an identity for the
volume integral of the square of a vector field that was quoted by Gubarev,
Stodolsky and Zakharov. In this comment, I provide a momentum-space derivation
of this result, generalized to the scalar product of two complex vector fields.
This approa... | physics.class-ph physics.ed-ph | stewart has provided a positionspace derivation of an identity for the volume integral of the square of a vector field that was quoted by gubarev stodolsky and zakharov in this comment i provide a momentumspace derivation of this result generalized to the scalar product of two complex vector fields this approach demons... | [['stewart', 'has', 'provided', 'a', 'positionspace', 'derivation', 'of', 'an', 'identity', 'for', 'the', 'volume', 'integral', 'of', 'the', 'square', 'of', 'a', 'vector', 'field', 'that', 'was', 'quoted', 'by', 'gubarev', 'stodolsky', 'and', 'zakharov', 'in', 'this', 'comment', 'i', 'provide', 'a', 'momentumspace', 'd... | [-0.13893370526946253, 0.0725481029320589, -0.1340773881206082, 0.06426198394587522, -0.10212650401000348, -0.07148743859337021, 0.020865690121556528, 0.2864949446844144, -0.21353514471815693, -0.2500320973599123, 0.07720797958124119, -0.21380622520680642, -0.17596110212616622, 0.19497583096057902, -0.01734299722334577... |
707.4133 | Multiuser Successive Refinement and Multiple Description Coding | We consider the multiuser successive refinement (MSR) problem, where the
users are connected to a central server via links with different noiseless
capacities, and each user wishes to reconstruct in a successive-refinement
fashion. An achievable region is given for the two-user two-layer case and it
provides the comp... | cs.IT math.IT | we consider the multiuser successive refinement msr problem where the users are connected to a central server via links with different noiseless capacities and each user wishes to reconstruct in a successiverefinement fashion an achievable region is given for the twouser twolayer case and it provides the complete rated... | [['we', 'consider', 'the', 'multiuser', 'successive', 'refinement', 'msr', 'problem', 'where', 'the', 'users', 'are', 'connected', 'to', 'a', 'central', 'server', 'via', 'links', 'with', 'different', 'noiseless', 'capacities', 'and', 'each', 'user', 'wishes', 'to', 'reconstruct', 'in', 'a', 'successiverefinement', 'fas... | [-0.13630323125149946, 0.009841702572764207, -0.07829270128564546, 0.06588383629788641, -0.06339985608369961, -0.20030853885353478, 0.07328131191502035, 0.38491871905864766, -0.3195123440301996, -0.24631198463551854, 0.12340899143576683, -0.27191343552073566, -0.16234129243066603, 0.1790023589727983, -0.122322367945023... |
707.4134 | Splicing and the SL(2,C) Casson invariant | We establish a formula for the SL(2,C) Casson invariant of spliced sums of
homology spheres along knots. Along the way, we show that the SL(2,C) Casson
invariant vanishes for spliced sums along knots in the 3-sphere.
| math.GT | we establish a formula for the sl2c casson invariant of spliced sums of homology spheres along knots along the way we show that the sl2c casson invariant vanishes for spliced sums along knots in the 3sphere | [['we', 'establish', 'a', 'formula', 'for', 'the', 'sl2c', 'casson', 'invariant', 'of', 'spliced', 'sums', 'of', 'homology', 'spheres', 'along', 'knots', 'along', 'the', 'way', 'we', 'show', 'that', 'the', 'sl2c', 'casson', 'invariant', 'vanishes', 'for', 'spliced', 'sums', 'along', 'knots', 'in', 'the', '3sphere']] | [-0.3787333222830461, 0.10619010558972757, -0.18022575845114058, 0.09850452000844395, -0.07677358497555058, -0.1399372474471521, -0.027051349222246144, 0.39647472608420586, -0.3191273807703207, -0.20239052766313156, 0.024926605010275833, -0.22808851436194447, -0.1689302229658804, 0.1737270707057582, -0.1490518184016562... |
707.4135 | A landing theorem for dynamic rays of geometrically finite entire
functions | A transcendental entire function f is called geometrically finite if the
intersection of the set of singular values with the Fatou set is compact and
the intersection of the postsingular set with the Julia set is finite. (In
particular, this includes all entire functions with finite postsingular set.)
If f is geometr... | math.DS | a transcendental entire function f is called geometrically finite if the intersection of the set of singular values with the fatou set is compact and the intersection of the postsingular set with the julia set is finite in particular this includes all entire functions with finite postsingular set if f is geometrically ... | [['a', 'transcendental', 'entire', 'function', 'f', 'is', 'called', 'geometrically', 'finite', 'if', 'the', 'intersection', 'of', 'the', 'set', 'of', 'singular', 'values', 'with', 'the', 'fatou', 'set', 'is', 'compact', 'and', 'the', 'intersection', 'of', 'the', 'postsingular', 'set', 'with', 'the', 'julia', 'set', 'is... | [-0.19966652528627923, 0.1344389793392015, -0.11048507043099227, 0.011199902682595788, -0.07366435995362208, -0.11885226689168792, 0.02357555501236531, 0.32659602125395876, -0.3405969331139012, -0.13430698847744343, 0.09863080208857641, -0.3171966452925852, -0.09335835966569568, 0.20855572172838852, -0.0740245294123030... |
707.4136 | Gauge Theory in Two Dimensions: Topological, Geometric and Probabilistic
Aspects | We present a description of two dimensional Yang-Mills gauge theory on the
plane and on compact surfaces, examining the topological, geometric and
probabilistic aspects.
| hep-th math-ph math.MP | we present a description of two dimensional yangmills gauge theory on the plane and on compact surfaces examining the topological geometric and probabilistic aspects | [['we', 'present', 'a', 'description', 'of', 'two', 'dimensional', 'yangmills', 'gauge', 'theory', 'on', 'the', 'plane', 'and', 'on', 'compact', 'surfaces', 'examining', 'the', 'topological', 'geometric', 'and', 'probabilistic', 'aspects']] | [-0.16566630970919505, 0.13700488120472679, -0.1221814441960305, 0.09741469860697786, -0.08829172188416123, -0.06264565976258989, 0.022668484331613097, 0.3612333884617935, -0.14959589067924148, -0.22406276959615448, 0.08549036844245468, -0.2419604476696501, -0.23482473815480867, 0.18555607475961247, -0.0799934013048186... |
707.4137 | Measurement of the slope parameter \alpha for the \eta\to 3\pi^0 decay
at KLOE | We report a preliminary measurement of the slope parameter $\alpha$ for the
$\eta\to 3\piz$ decay carried out with KLOE at DA$\Phi$NE; where $\alpha$ is
the parameter describing the energy dependence of the square of the matrix
element for this decay. By fitting the event density in the Dalitz plot with a
collected s... | hep-ex | we report a preliminary measurement of the slope parameter alpha for the etato 3piz decay carried out with kloe at daphine where alpha is the parameter describing the energy dependence of the square of the matrix element for this decay by fitting the event density in the dalitz plot with a collected statistic of 420 pb... | [['we', 'report', 'a', 'preliminary', 'measurement', 'of', 'the', 'slope', 'parameter', 'alpha', 'for', 'the', 'etato', '3piz', 'decay', 'carried', 'out', 'with', 'kloe', 'at', 'daphine', 'where', 'alpha', 'is', 'the', 'parameter', 'describing', 'the', 'energy', 'dependence', 'of', 'the', 'square', 'of', 'the', 'matrix... | [-0.08241215068242186, 0.16806961764133982, -0.12771408173993423, 0.02083625981293909, 0.0006541498549669593, -0.1138212608850815, 0.0625148939782173, 0.29351555171434757, -0.17206494135679315, -0.34065816178086344, 0.014397669969090298, -0.3748834277079864, 0.009727804062815456, 0.14424917630113468, 0.0591464569737723... |
707.4138 | Alkali Line Profiles in Ultracool White Dwarfs | We present PHOENIX atmosphere models for metal-rich cool white dwarfs using
improved line shapes for the Na I and K I resonance doublets. Profiles for
collisional broadening due to H2 and He based on the adiabatic representation
show strong deviations from Van der Waals interaction at short distances.
Comparison with... | astro-ph | we present phoenix atmosphere models for metalrich cool white dwarfs using improved line shapes for the na i and k i resonance doublets profiles for collisional broadening due to h2 and he based on the adiabatic representation show strong deviations from van der waals interaction at short distances comparison with obse... | [['we', 'present', 'phoenix', 'atmosphere', 'models', 'for', 'metalrich', 'cool', 'white', 'dwarfs', 'using', 'improved', 'line', 'shapes', 'for', 'the', 'na', 'i', 'and', 'k', 'i', 'resonance', 'doublets', 'profiles', 'for', 'collisional', 'broadening', 'due', 'to', 'h2', 'and', 'he', 'based', 'on', 'the', 'adiabatic'... | [-0.0328650176959207, 0.1178218300418062, -0.05986298841174684, 0.13007433360720733, -0.10042919992208797, -0.09962376260782703, 0.06084168415765231, 0.37870720556495174, -0.13465892199932014, -0.3483881791658952, 0.013292230004681495, -0.289430396406422, -0.04617547155042195, 0.1802597765433918, -0.04307007023441148, ... |
707.4139 | Heavy-quark production in gluon fusion at two loops in QCD | We present the two-loop virtual QCD corrections to the production of heavy
quarks in gluon fusion. The results are exact in the limit when all kinematical
invariants are large compared to the mass of the heavy quark up to terms
suppressed by powers of the heavy-quark mass. Our derivation uses a simple
relation betwee... | hep-ph | we present the twoloop virtual qcd corrections to the production of heavy quarks in gluon fusion the results are exact in the limit when all kinematical invariants are large compared to the mass of the heavy quark up to terms suppressed by powers of the heavyquark mass our derivation uses a simple relation between mass... | [['we', 'present', 'the', 'twoloop', 'virtual', 'qcd', 'corrections', 'to', 'the', 'production', 'of', 'heavy', 'quarks', 'in', 'gluon', 'fusion', 'the', 'results', 'are', 'exact', 'in', 'the', 'limit', 'when', 'all', 'kinematical', 'invariants', 'are', 'large', 'compared', 'to', 'the', 'mass', 'of', 'the', 'heavy', 'q... | [-0.0801725723547861, 0.2454169420339167, -0.08518060903530568, 0.13581560735125095, -0.030639506014995276, -0.021023880755528808, 0.01786775455926545, 0.31228120060637593, -0.14849208665080368, -0.23917837435379624, -0.01887810245505534, -0.340978847136721, -0.01304055861197412, 0.14089555874466897, 0.0860363032901659... |
707.414 | Non-annulation effective et positivit\'e locale des fibr\'es en droites
amples adjoints | We prove that Seshadri constants of some ample divisors are bigger than 1 on
smooth threefolds whose anticanonical bundle is nef or on Fano varieties of
small coindice. The main tools are (some known cases of) the Kawamata's
effective non-vanishing conjecture and the adjunction theory. We prove the
non-vanishing conj... | math.AG | we prove that seshadri constants of some ample divisors are bigger than 1 on smooth threefolds whose anticanonical bundle is nef or on fano varieties of small coindice the main tools are some known cases of the kawamatas effective nonvanishing conjecture and the adjunction theory we prove the nonvanishing conjecture in... | [['we', 'prove', 'that', 'seshadri', 'constants', 'of', 'some', 'ample', 'divisors', 'are', 'bigger', 'than', '1', 'on', 'smooth', 'threefolds', 'whose', 'anticanonical', 'bundle', 'is', 'nef', 'or', 'on', 'fano', 'varieties', 'of', 'small', 'coindice', 'the', 'main', 'tools', 'are', 'some', 'known', 'cases', 'of', 'th... | [-0.24779524167713066, 0.02752098487958742, -0.039320587280851145, 0.1544266307959333, -0.06973384477627965, -0.2559432403972516, -0.011188740202655586, 0.3139938459086877, -0.2276076663643695, -0.17337231936936195, 0.10790828550592638, -0.2718404108730073, -0.16705494004015167, 0.23565640207021854, -0.2109669105078165... |
707.4141 | Resolution of symplectic cyclic orbifold singularities | In this paper we present a method to obtain resolutions of symplectic
orbifolds arising from symplectic reduction of a Hamiltonian S^1-manifold at a
regular value. As an application, we show that all isolated cyclic
singularities of a symplectic orbifold admit a resolution and that
pre-quantisations of symplectic orb... | math.SG | in this paper we present a method to obtain resolutions of symplectic orbifolds arising from symplectic reduction of a hamiltonian s1manifold at a regular value as an application we show that all isolated cyclic singularities of a symplectic orbifold admit a resolution and that prequantisations of symplectic orbifolds ... | [['in', 'this', 'paper', 'we', 'present', 'a', 'method', 'to', 'obtain', 'resolutions', 'of', 'symplectic', 'orbifolds', 'arising', 'from', 'symplectic', 'reduction', 'of', 'a', 'hamiltonian', 's1manifold', 'at', 'a', 'regular', 'value', 'as', 'an', 'application', 'we', 'show', 'that', 'all', 'isolated', 'cyclic', 'sin... | [-0.2124792215483332, 0.012941509754994142, -0.13608589708908564, 0.08550250476346938, -0.084319508039496, -0.15926544266511444, -0.05055118476566686, 0.3743125772862523, -0.2533127083270638, -0.22685721590770064, 0.10094328872057506, -0.2235469558034782, -0.2024516933080223, 0.17677755545203885, -0.21011355255420008, ... |
707.4142 | On possible implications of gluon number fluctuations in DIS data | We study the effect of gluon number fluctuations (Pomeron loops) on deep
inelastic scattering (DIS) in the fixed coupling case. We find that the
description of the DIS data is improved once gluon number fluctuations are
included. Also the values of the parameters, like the saturation exponent and
the diffussion coeff... | hep-ph | we study the effect of gluon number fluctuations pomeron loops on deep inelastic scattering dis in the fixed coupling case we find that the description of the dis data is improved once gluon number fluctuations are included also the values of the parameters like the saturation exponent and the diffussion coefficient tu... | [['we', 'study', 'the', 'effect', 'of', 'gluon', 'number', 'fluctuations', 'pomeron', 'loops', 'on', 'deep', 'inelastic', 'scattering', 'dis', 'in', 'the', 'fixed', 'coupling', 'case', 'we', 'find', 'that', 'the', 'description', 'of', 'the', 'dis', 'data', 'is', 'improved', 'once', 'gluon', 'number', 'fluctuations', 'a... | [-0.11501915719791138, 0.16866099677810614, -0.15083276344971222, 0.14035085108215836, -0.06871930263168756, -0.05399726680287522, 0.06269980955499509, 0.3033517836323701, -0.23154633979059078, -0.2704195773367547, 0.055656547459950745, -0.3161609020730681, -0.08659579275822467, 0.17229174955340087, 0.03014533521515155... |
707.4143 | Hopf algebra of non-commutative field theory | We contruct here the Hopf algebra structure underlying the process of
renormalization of non-commutative quantum field theory.
| math-ph hep-th math.MP math.QA | we contruct here the hopf algebra structure underlying the process of renormalization of noncommutative quantum field theory | [['we', 'contruct', 'here', 'the', 'hopf', 'algebra', 'structure', 'underlying', 'the', 'process', 'of', 'renormalization', 'of', 'noncommutative', 'quantum', 'field', 'theory']] | [-0.19609186658635736, 0.15722814054392717, -0.1708626339540762, 0.08290388091753652, -0.15643664865809329, -0.09673881541718454, -0.014937406234607539, 0.3327574991785428, -0.45667291213484373, -0.16370849968755946, 0.08900070132906823, -0.14957773071878097, -0.29265491445274916, 0.09520001178059508, -0.04423140786478... |
707.4144 | The grid-dose-spreading algorithm for dose distribution calculation in
heavy charged particle radiotherapy | A new variant of the pencil-beam (PB) algorithm for dose distribution
calculation for radiotherapy with protons and heavier ions, the grid-dose
spreading (GDS) algorithm, is proposed. The GDS algorithm is intrinsically
faster than conventional PB algorithms due to approximations in convolution
integral, where physica... | physics.med-ph | a new variant of the pencilbeam pb algorithm for dose distribution calculation for radiotherapy with protons and heavier ions the griddose spreading gds algorithm is proposed the gds algorithm is intrinsically faster than conventional pb algorithms due to approximations in convolution integral where physical calculatio... | [['a', 'new', 'variant', 'of', 'the', 'pencilbeam', 'pb', 'algorithm', 'for', 'dose', 'distribution', 'calculation', 'for', 'radiotherapy', 'with', 'protons', 'and', 'heavier', 'ions', 'the', 'griddose', 'spreading', 'gds', 'algorithm', 'is', 'proposed', 'the', 'gds', 'algorithm', 'is', 'intrinsically', 'faster', 'than... | [-0.011036456321855471, 0.08215927588358773, -0.05344043593948423, 0.06957729844807906, -0.018341379058626244, -0.16521295112798431, 0.02695897631189328, 0.4497603218434221, -0.221341257675493, -0.326556291604825, 0.04994092369649433, -0.24931697109661533, -0.04918937853374387, 0.22408263281245563, -0.06674450732199318... |
707.4145 | Flux tubes as the origin of Net Circular Polarization in Sunspot
Penumbrae | We employ a 3-dimensional magnetohydrostatic model of a horizontal flux tube,
embedded in a magnetic surrounding atmosphere, to successfully reproduce the
azimuthal and center-to-limb variations of the Net Circular Polarization
observed in sunspot penumbrae. This success is partly due to the realistic
modeling of the... | astro-ph | we employ a 3dimensional magnetohydrostatic model of a horizontal flux tube embedded in a magnetic surrounding atmosphere to successfully reproduce the azimuthal and centertolimb variations of the net circular polarization observed in sunspot penumbrae this success is partly due to the realistic modeling of the interac... | [['we', 'employ', 'a', '3dimensional', 'magnetohydrostatic', 'model', 'of', 'a', 'horizontal', 'flux', 'tube', 'embedded', 'in', 'a', 'magnetic', 'surrounding', 'atmosphere', 'to', 'successfully', 'reproduce', 'the', 'azimuthal', 'and', 'centertolimb', 'variations', 'of', 'the', 'net', 'circular', 'polarization', 'obse... | [-0.12530996049330992, 0.14844751068475573, -0.0005656526847319169, 0.11112264940007166, -0.040977461297403685, -0.002571062108671123, -0.04080608890137889, 0.4388787719336423, -0.21112815688618206, -0.3949349849738858, 0.03908048797483471, -0.20393289801749317, -0.0801959244445739, 0.13229033866135234, -0.065825685638... |
707.4146 | Forecasting the Evolution of Dynamical Systems from Noisy Observations | We consider the problem of designing almost optimal predictors for dynamical
systems from a finite sequence of noisy observations and incomplete knowledge
of the dynamics and the noise. We first discuss the properties of the optimal
(Bayes) predictor and present the limitations of memory-free forecasting
methods, and... | nlin.CD | we consider the problem of designing almost optimal predictors for dynamical systems from a finite sequence of noisy observations and incomplete knowledge of the dynamics and the noise we first discuss the properties of the optimal bayes predictor and present the limitations of memoryfree forecasting methods and of any... | [['we', 'consider', 'the', 'problem', 'of', 'designing', 'almost', 'optimal', 'predictors', 'for', 'dynamical', 'systems', 'from', 'a', 'finite', 'sequence', 'of', 'noisy', 'observations', 'and', 'incomplete', 'knowledge', 'of', 'the', 'dynamics', 'and', 'the', 'noise', 'we', 'first', 'discuss', 'the', 'properties', 'o... | [-0.10329022712033728, 0.06277558494602209, -0.09177592461523802, 0.1048804907867199, -0.0599291519747804, -0.12860550291066908, 0.07769119900970153, 0.39998206450887347, -0.3122978946922914, -0.2606813328097696, 0.12402716883073521, -0.2515363748225829, -0.19795193327995747, 0.19225130558580808, -0.09174183942377567, ... |
707.4147 | The role of thermal evaporation in galaxy formation | In colour-magnitude diagrams most galaxies fall in either the ``blue cloud''
or the ``red sequence'', with the red sequence extending to significantly
brighter magnitudes than the blue cloud. The bright-end of the red sequence
comprises elliptical galaxies (Es) with boxy isophotes and luminosity profiles
with shallow... | astro-ph | in colourmagnitude diagrams most galaxies fall in either the blue cloud or the red sequence with the red sequence extending to significantly brighter magnitudes than the blue cloud the brightend of the red sequence comprises elliptical galaxies es with boxy isophotes and luminosity profiles with shallow central cores w... | [['in', 'colourmagnitude', 'diagrams', 'most', 'galaxies', 'fall', 'in', 'either', 'the', 'blue', 'cloud', 'or', 'the', 'red', 'sequence', 'with', 'the', 'red', 'sequence', 'extending', 'to', 'significantly', 'brighter', 'magnitudes', 'than', 'the', 'blue', 'cloud', 'the', 'brightend', 'of', 'the', 'red', 'sequence', '... | [-0.038594532720562, 0.14118545893916412, -0.10290612829780645, 0.12006262809074685, -0.05558817476928964, -0.054462753123530716, 0.004729793281477017, 0.4309737330119984, -0.09528692371358036, -0.3328509294994029, 0.013915954695046678, -0.3011898354718498, 0.003788865177079524, 0.16965584029516606, -0.0612446989069747... |
707.4148 | Search for phi to K0 K0bar gamma decay with KLOE | The KLOE collaboration has searched for the phi to K0 K0bar gamma decay using
a sample of 1.4 fb-1 of e+e- collisions at W ~ M(phi) collected with the KLOE
experiment at the Frascati e+e- collider DAFNE. No previous search exists for
this decay, while many theory models predict a BR of 10-8 for this channel. We
set a... | hep-ex | the kloe collaboration has searched for the phi to k0 k0bar gamma decay using a sample of 14 fb1 of ee collisions at w mphi collected with the kloe experiment at the frascati ee collider dafne no previous search exists for this decay while many theory models predict a br of 108 for this channel we set a preliminary val... | [['the', 'kloe', 'collaboration', 'has', 'searched', 'for', 'the', 'phi', 'to', 'k0', 'k0bar', 'gamma', 'decay', 'using', 'a', 'sample', 'of', '14', 'fb1', 'of', 'ee', 'collisions', 'at', 'w', 'mphi', 'collected', 'with', 'the', 'kloe', 'experiment', 'at', 'the', 'frascati', 'ee', 'collider', 'dafne', 'no', 'previous',... | [-0.08968883461202495, 0.10953992598806508, -0.09390240249340423, 0.048190905287628996, -0.014638772170292214, -0.15326157466624862, 0.13078395096526946, 0.3025964847241994, -0.17594714494916844, -0.2830222402539221, 0.011610090493923053, -0.41350589618086814, 0.06697029128554277, 0.17598210476135137, 0.139073519903467... |
707.4149 | Test configurations and Geodesic rays | For smooth test configurations, there always exist C^{1,1} geodesic rays in
Kahler metric space parallel to the algebraic ray. The $\yen$ invariant agrees
with Futaki invariant, at least under nice assumptions. Explicit examples in
Toric cases are calculated. On simple test configurations, Donaldson's
correspondence ... | math.DG math.AG | for smooth test configurations there always exist c11 geodesic rays in kahler metric space parallel to the algebraic ray the yen invariant agrees with futaki invariant at least under nice assumptions explicit examples in toric cases are calculated on simple test configurations donaldsons correspondence between hcma sol... | [['for', 'smooth', 'test', 'configurations', 'there', 'always', 'exist', 'c11', 'geodesic', 'rays', 'in', 'kahler', 'metric', 'space', 'parallel', 'to', 'the', 'algebraic', 'ray', 'the', 'yen', 'invariant', 'agrees', 'with', 'futaki', 'invariant', 'at', 'least', 'under', 'nice', 'assumptions', 'explicit', 'examples', '... | [-0.19813008609948293, 0.02946342954429675, -0.07931514107182903, 0.20858883539012651, -0.10632894165321903, -0.2006342342509976, -0.0655879696374232, 0.40846089249090206, -0.22435476185472789, -0.22586782083337037, 0.05011576429483885, -0.2616653532088506, -0.09913353149269549, 0.23594630017595472, -0.1291151081897177... |
707.415 | IAU Symposium 241 - Stellar Populations as Building Blocks of Galaxies | Stellar populations, building blocks of galaxies, are direct tracers of the
star formation history, the chemical enrichment and the assembly of galaxies in
the Universe. They therfore allow us to understand how galaxies formed and
evolved. This last decade has witnessed a revolution in our observations of
galaxies; w... | astro-ph | stellar populations building blocks of galaxies are direct tracers of the star formation history the chemical enrichment and the assembly of galaxies in the universe they therfore allow us to understand how galaxies formed and evolved this last decade has witnessed a revolution in our observations of galaxies with larg... | [['stellar', 'populations', 'building', 'blocks', 'of', 'galaxies', 'are', 'direct', 'tracers', 'of', 'the', 'star', 'formation', 'history', 'the', 'chemical', 'enrichment', 'and', 'the', 'assembly', 'of', 'galaxies', 'in', 'the', 'universe', 'they', 'therfore', 'allow', 'us', 'to', 'understand', 'how', 'galaxies', 'fo... | [-0.02824592358476935, 0.08926912919259188, -0.11842049569068425, 0.12103112834387371, -0.12982013494338238, -0.0495951354540052, 0.0358891508687683, 0.42109597991506814, -0.1743119003279811, -0.3666570057296428, 0.046832465341018106, -0.2639572878574527, -0.07076970716241185, 0.20506592957477227, -0.06485816930009666,... |
707.4151 | Studies of Drell-Yan dimuon events in the CMS experiment | The potential of the Compact Muon Solenoid (CMS) experiment to measure
Drell-Yan muon pairs is discussed. Muon pairs can be measured in CMS with high
precision up to very high invariant masses. The systematic errors are
considered. The potential to carry out precise measurements of the
forward-backward asymmetry is d... | hep-ex | the potential of the compact muon solenoid cms experiment to measure drellyan muon pairs is discussed muon pairs can be measured in cms with high precision up to very high invariant masses the systematic errors are considered the potential to carry out precise measurements of the forwardbackward asymmetry is discussed | [['the', 'potential', 'of', 'the', 'compact', 'muon', 'solenoid', 'cms', 'experiment', 'to', 'measure', 'drellyan', 'muon', 'pairs', 'is', 'discussed', 'muon', 'pairs', 'can', 'be', 'measured', 'in', 'cms', 'with', 'high', 'precision', 'up', 'to', 'very', 'high', 'invariant', 'masses', 'the', 'systematic', 'errors', 'a... | [-0.11983827464282512, 0.22401091382838786, -0.040826586298644545, 0.17912522973958403, -0.06458570640534163, -0.12892846006900072, -0.0031488874554634096, 0.36483840458095074, -0.21501598156057297, -0.3320617726445198, 0.018660594287794083, -0.3720629674196243, 0.13183404624462128, 0.22034495474770666, -0.018995757550... |
707.4152 | Stable two-channel Kondo fixed point of an SU(3) quantum defect in a
metal: renormalization group analysis and conductance spikes | We propose a physical realization of the two-channel Kondo (2CK) effect,
where a dynamical defect in a metal has a unique ground state and twofold
degenerate excited states. In a wide range of parameters the interactions with
the electrons renormalize the excited double downward below the bare defect
ground state, th... | cond-mat.mes-hall cond-mat.str-el | we propose a physical realization of the twochannel kondo 2ck effect where a dynamical defect in a metal has a unique ground state and twofold degenerate excited states in a wide range of parameters the interactions with the electrons renormalize the excited double downward below the bare defect ground state thus stabi... | [['we', 'propose', 'a', 'physical', 'realization', 'of', 'the', 'twochannel', 'kondo', '2ck', 'effect', 'where', 'a', 'dynamical', 'defect', 'in', 'a', 'metal', 'has', 'a', 'unique', 'ground', 'state', 'and', 'twofold', 'degenerate', 'excited', 'states', 'in', 'a', 'wide', 'range', 'of', 'parameters', 'the', 'interacti... | [-0.16843260177474068, 0.2497137310906305, -0.08249292913918711, 0.0661941437031822, -0.004914643515639745, -0.20967403760175682, 0.12086512616978169, 0.3256817112492213, -0.25605197833129417, -0.2658052996203706, -0.0036863025434122226, -0.3091956976180275, -0.11411947973894777, 0.1180109162898818, 0.03630768534567979... |
707.4153 | Opto-Mechanics of deformable Fabry-Perot Cavities | We investigated the opto-mechanical properties of a Fabry-Perot cavity with a
mirror mounted on a spring. Such a structure allows the cavity length to change
elastically under the effect of light induced forces. This opto-mechanical
coupling is exploited to control the amplitude of mechanical fluctuation of the
mirro... | cond-mat.other | we investigated the optomechanical properties of a fabryperot cavity with a mirror mounted on a spring such a structure allows the cavity length to change elastically under the effect of light induced forces this optomechanical coupling is exploited to control the amplitude of mechanical fluctuation of the mirror we pr... | [['we', 'investigated', 'the', 'optomechanical', 'properties', 'of', 'a', 'fabryperot', 'cavity', 'with', 'a', 'mirror', 'mounted', 'on', 'a', 'spring', 'such', 'a', 'structure', 'allows', 'the', 'cavity', 'length', 'to', 'change', 'elastically', 'under', 'the', 'effect', 'of', 'light', 'induced', 'forces', 'this', 'op... | [-0.20088475923591725, 0.17141740774394762, -0.12288014323148928, -0.013745873536862118, -0.06805817987507498, -0.14992660653292084, 0.031475308187253456, 0.3732893282783703, -0.28029448864325673, -0.26347605086548226, 0.05965647543944471, -0.24013546064293542, -0.15999388416678134, 0.24130663112737238, -0.049434523622... |
707.4154 | Remark on statistical model fits to particle ratios in relativistic
heavy ion collisions | In order to determine the chemical freeze-out parameters of the
hadron-emitting source in relativistic heavy ion collisions some studies in
literature perform fits by using as data input a subsample of ratios calculated
out of experimentally measured hadron yields instead of yields themselves. We
show that this is a ... | nucl-th | in order to determine the chemical freezeout parameters of the hadronemitting source in relativistic heavy ion collisions some studies in literature perform fits by using as data input a subsample of ratios calculated out of experimentally measured hadron yields instead of yields themselves we show that this is a stati... | [['in', 'order', 'to', 'determine', 'the', 'chemical', 'freezeout', 'parameters', 'of', 'the', 'hadronemitting', 'source', 'in', 'relativistic', 'heavy', 'ion', 'collisions', 'some', 'studies', 'in', 'literature', 'perform', 'fits', 'by', 'using', 'as', 'data', 'input', 'a', 'subsample', 'of', 'ratios', 'calculated', '... | [-0.05721517963240207, 0.10106782700424477, -0.1565645145473339, 0.11335010185711465, 0.0033653013060911227, -0.10436207562748154, 0.05650991668640557, 0.38392442221737516, -0.1952516802791822, -0.3522757574031919, -0.01908881944935706, -0.2988034528443369, 0.022348160413488492, 0.19903803322369518, 0.01728417796982547... |
707.4155 | XMM-Newton and INTEGRAL observations of the black hole candidate XTE
J1817-330 | The galactic black hole candidate XTE J1817-330 was discovered in outburst by
RXTE in January 2006. We present here the results of an XMM-Newton Target of
opportunity observation (TOO), performed on 13 March 2006 (44 days after the
maximum), and an INTEGRAL observation performed on 15-18 February 2006 (18 days
after ... | astro-ph | the galactic black hole candidate xte j1817330 was discovered in outburst by rxte in january 2006 we present here the results of an xmmnewton target of opportunity observation too performed on 13 march 2006 44 days after the maximum and an integral observation performed on 1518 february 2006 18 days after the maximum t... | [['the', 'galactic', 'black', 'hole', 'candidate', 'xte', 'j1817330', 'was', 'discovered', 'in', 'outburst', 'by', 'rxte', 'in', 'january', '2006', 'we', 'present', 'here', 'the', 'results', 'of', 'an', 'xmmnewton', 'target', 'of', 'opportunity', 'observation', 'too', 'performed', 'on', '13', 'march', '2006', '44', 'da... | [-0.054583362649298375, 0.10944927579956129, -0.054387647337797614, 0.056142877597465286, -0.07995872170457409, -0.0943067909570204, 0.07218071677896659, 0.4579198865137166, -0.15128311754463034, -0.38707458247948023, 0.11536275871305002, -0.38447201541935405, 0.021829730303078478, 0.2040680351180749, -0.02150168436654... |
707.4156 | Long-range fluctuations of random potential landscape as a mechanism of
1/f noise in hydrogenated amorphous silicon | We describe a mechanism, which links the long-range potential fluctuations
induced by charged defects to the low frequency resistance noise widely known
as 1/f noise. This mechanism is amenable to the first principles microscopic
calculation of the noise spectrum, which includes the absolute noise intensity.
We have ... | cond-mat.stat-mech cond-mat.dis-nn cond-mat.mtrl-sci | we describe a mechanism which links the longrange potential fluctuations induced by charged defects to the low frequency resistance noise widely known as 1f noise this mechanism is amenable to the first principles microscopic calculation of the noise spectrum which includes the absolute noise intensity we have performe... | [['we', 'describe', 'a', 'mechanism', 'which', 'links', 'the', 'longrange', 'potential', 'fluctuations', 'induced', 'by', 'charged', 'defects', 'to', 'the', 'low', 'frequency', 'resistance', 'noise', 'widely', 'known', 'as', '1f', 'noise', 'this', 'mechanism', 'is', 'amenable', 'to', 'the', 'first', 'principles', 'micr... | [-0.13767974713065345, 0.15348142653772043, -0.044359002142734485, 0.08012429852606814, 0.010081091207887876, -0.14793235658232226, 0.03283167494366954, 0.4037505037604122, -0.26196507000526703, -0.29195375494453885, 0.037882392885325765, -0.27485301643780885, -0.13869909074054945, 0.17548691062683905, -0.0318530572347... |
707.4157 | Phase Diagram of CeCoIn_5 in the Vicinity of H_{c2} as Determined by NMR | We report ^{115}In nuclear magnetic resonance (NMR) measurements in the
heavy-fermion superconductor CeCoIn_5 as a function of temperature in different
magnetic fields applied parallel to the $(\hat a, \hat b)$ plane. The
measurements probe a part of the phase diagram in the vicinity of the
superconducting critical f... | cond-mat.str-el cond-mat.supr-con | we report 115in nuclear magnetic resonance nmr measurements in the heavyfermion superconductor cecoin_5 as a function of temperature in different magnetic fields applied parallel to the hat a hat b plane the measurements probe a part of the phase diagram in the vicinity of the superconducting critical field h_c2 where ... | [['we', 'report', '115in', 'nuclear', 'magnetic', 'resonance', 'nmr', 'measurements', 'in', 'the', 'heavyfermion', 'superconductor', 'cecoin_5', 'as', 'a', 'function', 'of', 'temperature', 'in', 'different', 'magnetic', 'fields', 'applied', 'parallel', 'to', 'the', 'hat', 'a', 'hat', 'b', 'plane', 'the', 'measurements'... | [-0.20955320032363808, 0.2563410211178298, -0.06978977436980081, -0.007491900413328581, -0.04501832999930893, -0.1022971926376576, 0.122538043731962, 0.33805616249682735, -0.2237494619564402, -0.2730208718268251, 0.03473163426482446, -0.3131611512067753, -0.07940496546782654, 0.17257353891240987, 0.09263868831928719, 0... |
707.4158 | Spontaneous emission from a two--level atom tunneling in a double--well
potential | We study a two-level atom in a double--well potential coupled to a continuum
of electromagnetic modes (black body radiation in three dimensions at zero
absolute temperature). Internal and external degrees of the atom couple due to
recoil during emission of a photon. We provide a full analysis of the problem
in the lo... | quant-ph | we study a twolevel atom in a doublewell potential coupled to a continuum of electromagnetic modes black body radiation in three dimensions at zero absolute temperature internal and external degrees of the atom couple due to recoil during emission of a photon we provide a full analysis of the problem in the long wavele... | [['we', 'study', 'a', 'twolevel', 'atom', 'in', 'a', 'doublewell', 'potential', 'coupled', 'to', 'a', 'continuum', 'of', 'electromagnetic', 'modes', 'black', 'body', 'radiation', 'in', 'three', 'dimensions', 'at', 'zero', 'absolute', 'temperature', 'internal', 'and', 'external', 'degrees', 'of', 'the', 'atom', 'couple'... | [-0.13482837485241553, 0.19322896408207166, -0.050289345041545495, 0.037893353180395425, -0.006388854373484677, -0.12069039907967022, 0.08049153710368934, 0.383014349976208, -0.2581214280040978, -0.2878751027787667, 0.021477355312442322, -0.302100291453995, -0.020982810894438868, 0.16669981838691286, 0.0113424623471706... |
707.4159 | Density theorems for bipartite graphs and related Ramsey-type results | In this paper, we present several density-type theorems which show how to
find a copy of a sparse bipartite graph in a graph of positive density. Our
results imply several new bounds for classical problems in graph Ramsey theory
and improve and generalize earlier results of various researchers. The proofs
combine pro... | math.CO | in this paper we present several densitytype theorems which show how to find a copy of a sparse bipartite graph in a graph of positive density our results imply several new bounds for classical problems in graph ramsey theory and improve and generalize earlier results of various researchers the proofs combine probabili... | [['in', 'this', 'paper', 'we', 'present', 'several', 'densitytype', 'theorems', 'which', 'show', 'how', 'to', 'find', 'a', 'copy', 'of', 'a', 'sparse', 'bipartite', 'graph', 'in', 'a', 'graph', 'of', 'positive', 'density', 'our', 'results', 'imply', 'several', 'new', 'bounds', 'for', 'classical', 'problems', 'in', 'gra... | [-0.08371503013333348, 0.0916254875603421, -0.12437040204631872, 0.10003377710624288, -0.1284538471172082, -0.1235548725522969, 0.07300256865216825, 0.3701447780490264, -0.2773015350424524, -0.3297633416094314, 0.12397554544089683, -0.2685803769734399, -0.2129690201722899, 0.19025099599444917, -0.1481717660536069, 0.06... |
707.416 | Finite vertex algebras and nilpotence | I show that simple finite vertex algebras are commutative, and that the Lie
conformal algebra structure underlying a reduced (i.e., without nilpotent
elements) finite vertex algebra is nilpotent.
| math.QA | i show that simple finite vertex algebras are commutative and that the lie conformal algebra structure underlying a reduced ie without nilpotent elements finite vertex algebra is nilpotent | [['i', 'show', 'that', 'simple', 'finite', 'vertex', 'algebras', 'are', 'commutative', 'and', 'that', 'the', 'lie', 'conformal', 'algebra', 'structure', 'underlying', 'a', 'reduced', 'ie', 'without', 'nilpotent', 'elements', 'finite', 'vertex', 'algebra', 'is', 'nilpotent']] | [-0.14830647369048425, 0.17112982339624846, -0.02243574908269303, 0.02536093332621801, -0.30227225799379603, -0.2369976859772578, -0.11874537336240922, 0.40600617908473524, -0.4245857554487884, -0.07627099782361516, 0.11805129789614252, -0.2504507186489978, -0.12790753437937902, 0.046329812080200226, -0.148071085597621... |
707.4161 | Magnetic Field Generation in Planets and Satellites by Natural Nuclear
Fission Reactors | One of the most fundamental problems in physics has been to understand the
nature of the mechanism that generates the geomagnetic field and the magnetic
fields of other planets and satellites. For decades, the dynamo mechanism,
thought to be responsible for generating the geomagnetic field and other
planetary magneti... | physics.geo-ph physics.gen-ph physics.space-ph | one of the most fundamental problems in physics has been to understand the nature of the mechanism that generates the geomagnetic field and the magnetic fields of other planets and satellites for decades the dynamo mechanism thought to be responsible for generating the geomagnetic field and other planetary magnetic fie... | [['one', 'of', 'the', 'most', 'fundamental', 'problems', 'in', 'physics', 'has', 'been', 'to', 'understand', 'the', 'nature', 'of', 'the', 'mechanism', 'that', 'generates', 'the', 'geomagnetic', 'field', 'and', 'the', 'magnetic', 'fields', 'of', 'other', 'planets', 'and', 'satellites', 'for', 'decades', 'the', 'dynamo'... | [-0.09991842356595679, 0.23008498640158792, -0.052063646473696615, 0.0979758262332967, -0.07445978565146123, -0.040564832779779736, -0.011648952504437343, 0.28015737575204935, -0.2541244210883841, -0.3223209087706469, 0.05214689222843161, -0.21574179936516907, -0.12389826281239687, 0.2174938171006301, -0.04358602726217... |
707.4162 | Charmonium excited state spectrum in lattice QCD | Working with a large basis of covariant derivative-based meson interpolating
fields we demonstrate the feasibility of reliably extracting multiple excited
states using a variational method. The study is performed on quenched
anisotropic lattices with clover quarks at the charm mass. We demonstrate how a
knowledge of ... | hep-lat hep-ph | working with a large basis of covariant derivativebased meson interpolating fields we demonstrate the feasibility of reliably extracting multiple excited states using a variational method the study is performed on quenched anisotropic lattices with clover quarks at the charm mass we demonstrate how a knowledge of the c... | [['working', 'with', 'a', 'large', 'basis', 'of', 'covariant', 'derivativebased', 'meson', 'interpolating', 'fields', 'we', 'demonstrate', 'the', 'feasibility', 'of', 'reliably', 'extracting', 'multiple', 'excited', 'states', 'using', 'a', 'variational', 'method', 'the', 'study', 'is', 'performed', 'on', 'quenched', 'a... | [-0.10863343545102648, 0.22929261950332494, -0.1079078424455864, 0.09960371664436977, -0.022314033497657093, -0.0992037289642862, 0.10865231025077048, 0.39968089276836033, -0.19554107328987724, -0.2747657616916556, 0.06674496248098356, -0.2688213530196143, -0.05103532889015263, 0.09713908847022269, 0.06495668570111905,... |
707.4163 | Amplitudes in pp and p-pbar scattering | Solutions for the amplitudes that give accurate description of pp and p-pbar
scattering at high energies are investigated, with particular attention given
to the properties of their zeros and slopes, whose determination is required
for the study of the Coulomb interference region. Proper extrapolations of
these quant... | hep-ph | solutions for the amplitudes that give accurate description of pp and ppbar scattering at high energies are investigated with particular attention given to the properties of their zeros and slopes whose determination is required for the study of the coulomb interference region proper extrapolations of these quantities ... | [['solutions', 'for', 'the', 'amplitudes', 'that', 'give', 'accurate', 'description', 'of', 'pp', 'and', 'ppbar', 'scattering', 'at', 'high', 'energies', 'are', 'investigated', 'with', 'particular', 'attention', 'given', 'to', 'the', 'properties', 'of', 'their', 'zeros', 'and', 'slopes', 'whose', 'determination', 'is',... | [-0.09900970499341687, 0.13926598162700732, -0.08466295869244883, 0.12507401471375487, -0.02174914302304387, -0.06649558738184472, 0.008341310935793444, 0.3666522992425598, -0.16902793070767075, -0.3112269289481143, 0.06002839599386789, -0.3192732461417715, -0.04034090975377088, 0.2041625163828333, 0.07236483512630608,... |
707.4164 | Any-order propagation of the nonlinear Schroedinger equation | We derive an exact propagation scheme for nonlinear Schroedinger equations.
This scheme is entirely analogous to the propagation of linear Schroedinger
equations. We accomplish this by defining a special operator whose algebraic
properties ensure the correct propagation. As applications, we provide a simple
proof of ... | quant-ph | we derive an exact propagation scheme for nonlinear schroedinger equations this scheme is entirely analogous to the propagation of linear schroedinger equations we accomplish this by defining a special operator whose algebraic properties ensure the correct propagation as applications we provide a simple proof of a rece... | [['we', 'derive', 'an', 'exact', 'propagation', 'scheme', 'for', 'nonlinear', 'schroedinger', 'equations', 'this', 'scheme', 'is', 'entirely', 'analogous', 'to', 'the', 'propagation', 'of', 'linear', 'schroedinger', 'equations', 'we', 'accomplish', 'this', 'by', 'defining', 'a', 'special', 'operator', 'whose', 'algebra... | [-0.14825745927753733, 0.026937685470981177, -0.13318857558961236, 0.0742678770242926, -0.17188994803312999, -0.14678860612825226, -0.027111760443145994, 0.2974973521681864, -0.30351167569395654, -0.2408073768297683, 0.06471710492606594, -0.192221686577619, -0.20196868137303572, 0.20662826047028734, -0.0302470722027234... |
707.4165 | The Opacity of Spiral Galaxy Disks VIII: Structure of the Cold ISM | The quantity of dust in a spiral disk can be estimated using the dust's
typical emission or the extinction of a known source. In this paper, we compare
two techniques, one based on emission and one on absorption, applied on
sections of fourteen disk galaxies. The two measurements reflect, respectively
the average and... | astro-ph | the quantity of dust in a spiral disk can be estimated using the dusts typical emission or the extinction of a known source in this paper we compare two techniques one based on emission and one on absorption applied on sections of fourteen disk galaxies the two measurements reflect respectively the average and apparent... | [['the', 'quantity', 'of', 'dust', 'in', 'a', 'spiral', 'disk', 'can', 'be', 'estimated', 'using', 'the', 'dusts', 'typical', 'emission', 'or', 'the', 'extinction', 'of', 'a', 'known', 'source', 'in', 'this', 'paper', 'we', 'compare', 'two', 'techniques', 'one', 'based', 'on', 'emission', 'and', 'one', 'on', 'absorptio... | [-0.04752467454185368, 0.08583147297009029, -0.08226483177841563, 0.08800372333072112, -0.036438927321005184, -0.0480215203910995, -0.004053146302440552, 0.47080389940613554, -0.20796517793885397, -0.33924056865800994, 0.06378570283569382, -0.2854349793340186, -0.0013302976940047593, 0.20037423143650313, -0.04293614873... |
707.4166 | Parsimony Principles for Software Components and Metalanguages | Software is a communication system. The usual topic of communication is
program behavior, as encoded by programs. Domain-specific libraries are
codebooks, domain-specific languages are coding schemes, and so forth. To turn
metaphor into method, we adapt toolsfrom information theory--the study of
efficient communicati... | cs.SE | software is a communication system the usual topic of communication is program behavior as encoded by programs domainspecific libraries are codebooks domainspecific languages are coding schemes and so forth to turn metaphor into method we adapt toolsfrom information theorythe study of efficient communicationto probe th... | [['software', 'is', 'a', 'communication', 'system', 'the', 'usual', 'topic', 'of', 'communication', 'is', 'program', 'behavior', 'as', 'encoded', 'by', 'programs', 'domainspecific', 'libraries', 'are', 'codebooks', 'domainspecific', 'languages', 'are', 'coding', 'schemes', 'and', 'so', 'forth', 'to', 'turn', 'metaphor'... | [-0.12164854153525084, 0.009878323338004218, -0.10672306552070142, 0.07745667878771201, -0.16401740204439394, -0.16545285472335916, 0.06673579152621743, 0.39297975555657305, -0.3186662737441818, -0.3354526895408829, 0.06592551755925848, -0.2555559476126089, -0.1644011318606014, 0.18189522833304686, -0.1146174125218143,... |
707.4167 | Gaps in the cloud cover? Comparing extinction measures in spiral disks | Dust in galaxies can be mapped by either the FIR/sub-mm emission, the optical
or infrared reddening of starlight, or the extinction of a known background
source. We compare two dust extinction measurements for a set of fifteen
sections in thirteen nearby galaxies, to determine the scale of the dusty ISM
responsible f... | astro-ph | dust in galaxies can be mapped by either the firsubmm emission the optical or infrared reddening of starlight or the extinction of a known background source we compare two dust extinction measurements for a set of fifteen sections in thirteen nearby galaxies to determine the scale of the dusty ism responsible for disk ... | [['dust', 'in', 'galaxies', 'can', 'be', 'mapped', 'by', 'either', 'the', 'firsubmm', 'emission', 'the', 'optical', 'or', 'infrared', 'reddening', 'of', 'starlight', 'or', 'the', 'extinction', 'of', 'a', 'known', 'background', 'source', 'we', 'compare', 'two', 'dust', 'extinction', 'measurements', 'for', 'a', 'set', 'o... | [-0.023653278184462, 0.0449891736324141, -0.08746340331113474, 0.10361302386471917, -0.05848899716723033, -0.03673117171909491, 0.03040445377542214, 0.45903172047639434, -0.17717629090925172, -0.3290916461031884, 0.04915038815868849, -0.3060738738795573, -0.05373309354657646, 0.1694174952191216, -0.0715033794880252, -0... |
707.4168 | The $qqqq\bar{q}$ components and the magnetic moments of the charmed and
the bottomed baryons | We give the explicit wave functions of the $qqqq\bar{q}$ components of the
C=+1, J=1/2 charmed baryons, $\Sigma_{c}$, $\Lambda_{c}$ and $\Xi_{c}^{a}$, and
calculate the magnetic moments by adding the 5q components contributions, and
we also compute the magnetic moments of the $\Sigma_{b}$ and $\Sigma_{b}^{*}$
baryons... | hep-ph | we give the explicit wave functions of the qqqqbarq components of the c1 j12 charmed baryons sigma_c lambda_c and xi_ca and calculate the magnetic moments by adding the 5q components contributions and we also compute the magnetic moments of the sigma_b and sigma_b baryons the influence of the additional light and stran... | [['we', 'give', 'the', 'explicit', 'wave', 'functions', 'of', 'the', 'qqqqbarq', 'components', 'of', 'the', 'c1', 'j12', 'charmed', 'baryons', 'sigma_c', 'lambda_c', 'and', 'xi_ca', 'and', 'calculate', 'the', 'magnetic', 'moments', 'by', 'adding', 'the', '5q', 'components', 'contributions', 'and', 'we', 'also', 'comput... | [-0.08745552226513004, 0.29304608760401607, -0.07913737164189417, 0.15745593591826038, -0.05894396250136197, -0.05249166779840986, 0.061252123403828594, 0.3034977692862352, -0.1966819878667593, -0.2549128897488117, -0.03983588193465645, -0.3565822622242073, 0.010931208563658099, 0.07415857773739845, 0.11510629589979847... |
707.4169 | Typicality Defended | Hartle and Srednicki have argued that there is no observational evidence
favoring our typicality. Here it is shown that such evidence does arise from
including the `normalization principle' requirement that the sum of the
likelihoods for all possible observations is normalized to unity in each
theory.
| hep-th | hartle and srednicki have argued that there is no observational evidence favoring our typicality here it is shown that such evidence does arise from including the normalization principle requirement that the sum of the likelihoods for all possible observations is normalized to unity in each theory | [['hartle', 'and', 'srednicki', 'have', 'argued', 'that', 'there', 'is', 'no', 'observational', 'evidence', 'favoring', 'our', 'typicality', 'here', 'it', 'is', 'shown', 'that', 'such', 'evidence', 'does', 'arise', 'from', 'including', 'the', 'normalization', 'principle', 'requirement', 'that', 'the', 'sum', 'of', 'the... | [-0.10012552246157809, 0.10698485947416528, -0.14321772189324963, 0.10997087242962468, -0.09260575160505655, -0.1191601702214583, 0.037099123251644654, 0.35750611737856397, -0.21122565063769402, -0.26761237726263376, 0.08188474256008782, -0.2912270017474404, -0.17767668894046676, 0.18476959977946852, -0.040132979518207... |
707.417 | The Cosmic Neutrino Background and the Age of the Universe | We discuss the cosmological degeneracy between the age of the Universe, the
Hubble parameter and the effective number of relativistic particles N_eff. We
show that independent determinations of the Hubble parameter H(z) as those
recently provided by Simon,Verde, Jimenez (2006), combined with other
cosmological data s... | astro-ph hep-ph | we discuss the cosmological degeneracy between the age of the universe the hubble parameter and the effective number of relativistic particles n_eff we show that independent determinations of the hubble parameter hz as those recently provided by simonverde jimenez 2006 combined with other cosmological data sets can pro... | [['we', 'discuss', 'the', 'cosmological', 'degeneracy', 'between', 'the', 'age', 'of', 'the', 'universe', 'the', 'hubble', 'parameter', 'and', 'the', 'effective', 'number', 'of', 'relativistic', 'particles', 'n_eff', 'we', 'show', 'that', 'independent', 'determinations', 'of', 'the', 'hubble', 'parameter', 'hz', 'as', ... | [-0.10599331893591267, 0.18781276886493103, -0.030574684661596713, 0.10107179488069519, -0.06812873303965487, -0.12363584634537499, 0.08407335147035844, 0.28005518591163137, -0.12571017762806003, -0.4406217735665239, 0.05229332896932545, -0.29489858255185414, 0.03688122168409102, 0.2108808650230669, 0.00579111992071072... |
707.4171 | Coulomb interaction, ripples, and the minimal conductivity of graphene | We argue that the unscreened Coulomb interaction in graphene provides a
positive, universal, and logarithmic correction to scaling of zero-temperature
conductivity with frequency. The combined effect of the disorder due to
wrinkling of the graphene sheet and the long range electron-electron
interactions is a finite p... | cond-mat.mes-hall cond-mat.str-el | we argue that the unscreened coulomb interaction in graphene provides a positive universal and logarithmic correction to scaling of zerotemperature conductivity with frequency the combined effect of the disorder due to wrinkling of the graphene sheet and the long range electronelectron interactions is a finite positive... | [['we', 'argue', 'that', 'the', 'unscreened', 'coulomb', 'interaction', 'in', 'graphene', 'provides', 'a', 'positive', 'universal', 'and', 'logarithmic', 'correction', 'to', 'scaling', 'of', 'zerotemperature', 'conductivity', 'with', 'frequency', 'the', 'combined', 'effect', 'of', 'the', 'disorder', 'due', 'to', 'wrink... | [-0.18839062777403584, 0.18454276613851822, -0.05520028617028067, 0.014539815480502434, -0.021768084729217693, -0.14002204711477345, 0.06172100944632593, 0.3145625739215085, -0.2855870997469522, -0.24322092878576526, 0.0033508218231841796, -0.3426127733471684, -0.14802218567128253, 0.14108246157709986, 0.03408569470445... |
707.4172 | Pairing states of a polarized Fermi gas trapped in a one-dimensional
optical lattice | We study the properties of a one-dimensional (1D) gas of fermions trapped in
a lattice by means of the density matrix renormalization group method, focusing
on the case of unequal spin populations, and strong attractive interaction. In
the low density regime, the system phase-separates into a well defined
superconduc... | cond-mat.str-el cond-mat.supr-con | we study the properties of a onedimensional 1d gas of fermions trapped in a lattice by means of the density matrix renormalization group method focusing on the case of unequal spin populations and strong attractive interaction in the low density regime the system phaseseparates into a well defined superconducting core ... | [['we', 'study', 'the', 'properties', 'of', 'a', 'onedimensional', '1d', 'gas', 'of', 'fermions', 'trapped', 'in', 'a', 'lattice', 'by', 'means', 'of', 'the', 'density', 'matrix', 'renormalization', 'group', 'method', 'focusing', 'on', 'the', 'case', 'of', 'unequal', 'spin', 'populations', 'and', 'strong', 'attractive'... | [-0.19699316260262206, 0.2790383971693767, -0.0648981884956678, 0.023836585917373802, 3.003036154706667e-05, -0.14366770952531113, 0.08215790163642563, 0.362873441198977, -0.21401287693240703, -0.23079995041224743, 0.014268409648893128, -0.29512589129702, -0.020425647768339644, 0.11512266541121347, 0.07557929734480795,... |
707.4173 | A Wide-field Survey of Two Z~0.5 Galaxy Clusters: Identifying the
Physical Processes Responsible for the Observed Transformation of Spirals
into S0s | We present new results from our comprehensive comparative survey of two
massive, intermediate redshift galaxy clusters, Cl0024+17 (z=0.39) and
MS0451-03 (z=0.54). We identify and study several key classes of `transition
objects' whose stellar populations or dynamical states indicate a recent or
ongoing change in morp... | astro-ph | we present new results from our comprehensive comparative survey of two massive intermediate redshift galaxy clusters cl002417 z039 and ms045103 z054 we identify and study several key classes of transition objects whose stellar populations or dynamical states indicate a recent or ongoing change in morphology and star f... | [['we', 'present', 'new', 'results', 'from', 'our', 'comprehensive', 'comparative', 'survey', 'of', 'two', 'massive', 'intermediate', 'redshift', 'galaxy', 'clusters', 'cl002417', 'z039', 'and', 'ms045103', 'z054', 'we', 'identify', 'and', 'study', 'several', 'key', 'classes', 'of', 'transition', 'objects', 'whose', 's... | [-0.08172610500068576, 0.11594697138191097, -0.11542833376637039, 0.08603561880291737, -0.08270228901291611, -0.01007411265961343, 0.04210870421590732, 0.42752684035372956, -0.1937801507267135, -0.2989735509939406, 0.061510961101804346, -0.24047270060206452, -0.0903158917117657, 0.16813211783473553, 0.04021537288316284... |
707.4174 | Retinoblastoma protein is the likely common effector for distinct
anti-aging pathways | The multiple worlds of genetically manipulated laboratory organisms such as
transgenic mice or worms with certain gene mutations are somewhat reminiscent
of parallel worlds in quantum mechanics. So are various models of aging tested
in such organisms. In this context, the tumor suppressor p53 has been found to
either... | q-bio.SC q-bio.BM | the multiple worlds of genetically manipulated laboratory organisms such as transgenic mice or worms with certain gene mutations are somewhat reminiscent of parallel worlds in quantum mechanics so are various models of aging tested in such organisms in this context the tumor suppressor p53 has been found to either acce... | [['the', 'multiple', 'worlds', 'of', 'genetically', 'manipulated', 'laboratory', 'organisms', 'such', 'as', 'transgenic', 'mice', 'or', 'worms', 'with', 'certain', 'gene', 'mutations', 'are', 'somewhat', 'reminiscent', 'of', 'parallel', 'worlds', 'in', 'quantum', 'mechanics', 'so', 'are', 'various', 'models', 'of', 'ag... | [-0.04383700442874534, 0.15755119297303197, -0.05777759922859378, 0.08066547850970752, -0.03798100498154696, -0.18638744245434546, 0.01700408945982464, 0.3682375157204194, -0.24066345176349083, -0.2667291933893521, 0.050845678793226615, -0.24029663940254822, -0.2538334338241217, 0.2099749138777773, -0.12657081277475843... |
707.4175 | On Hadamard matrices at roots of unity | This paper has been withdrawn by the authors, the main result being known
since Lam and Leung, J. Algebra 2000.
| math.CO | this paper has been withdrawn by the authors the main result being known since lam and leung j algebra 2000 | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'the', 'main', 'result', 'being', 'known', 'since', 'lam', 'and', 'leung', 'j', 'algebra', '2000']] | [-0.09147017784416675, 0.004682807391509414, -0.06576270153746008, -0.04469173758407123, -0.12234678063541651, -0.1190218549920246, -0.02241276073618792, 0.27172873076051474, -0.2682449705898762, -0.3854289246723056, 0.17878573052585126, -0.2310625015757978, -0.15499034328386188, 0.10511438963003457, -0.296710630971938... |
707.4176 | Nuclear spirals as feeding channels to the Supermassive Black Hole: the
case of the galaxy NGC 6951 | We report the discovery of gas streaming motions along nuclear spiral arms
towards the LINER nucleus of the galaxy NGC 6951. The observations, obtained
using the GMOS integral field spectrograph on the Gemini North telescope,
yielded maps of the flux distributions and gas kinematics in the Halpha,
[NII]6584 and [SII]... | astro-ph | we report the discovery of gas streaming motions along nuclear spiral arms towards the liner nucleus of the galaxy ngc 6951 the observations obtained using the gmos integral field spectrograph on the gemini north telescope yielded maps of the flux distributions and gas kinematics in the halpha nii6584 and sii671731 emi... | [['we', 'report', 'the', 'discovery', 'of', 'gas', 'streaming', 'motions', 'along', 'nuclear', 'spiral', 'arms', 'towards', 'the', 'liner', 'nucleus', 'of', 'the', 'galaxy', 'ngc', '6951', 'the', 'observations', 'obtained', 'using', 'the', 'gmos', 'integral', 'field', 'spectrograph', 'on', 'the', 'gemini', 'north', 'te... | [-0.09423584430120312, 0.038023799610061526, -0.11270101532005729, 0.04803695692979277, -0.08384526540469538, -0.04044912785339432, -0.021050883668502714, 0.4207067673818933, -0.1864600208693415, -0.26332251597036666, 0.062464153945832074, -0.25107565209763044, 0.03262646223938801, 0.17691032021230835, -0.0038661462666... |
707.4177 | Coupling Between An Optical Phonon and the Kondo Effect | We explore the ultra-fast optical response of Yb_{14}MnSb_{11}, providing
further evidence that this Zintl compound is the first ferromagnetic,
under-screened Kondo lattice. These experiments also provide the first
demonstration of coupling between an optical phonon mode and the Kondo effect.
| cond-mat.str-el | we explore the ultrafast optical response of yb_14mnsb_11 providing further evidence that this zintl compound is the first ferromagnetic underscreened kondo lattice these experiments also provide the first demonstration of coupling between an optical phonon mode and the kondo effect | [['we', 'explore', 'the', 'ultrafast', 'optical', 'response', 'of', 'yb_14mnsb_11', 'providing', 'further', 'evidence', 'that', 'this', 'zintl', 'compound', 'is', 'the', 'first', 'ferromagnetic', 'underscreened', 'kondo', 'lattice', 'these', 'experiments', 'also', 'provide', 'the', 'first', 'demonstration', 'of', 'coup... | [-0.16893015400721476, 0.1833534413767316, -0.08637130403747925, 0.0021005327311845925, -0.08383012591646267, -0.149358667839223, 0.12084439585510737, 0.4349704782765072, -0.27644356524046415, -0.221452800079416, 0.009438426723369421, -0.3041738383471966, -0.20320226834752622, 0.1908239062445668, 0.12474697770980689, -... |
707.4178 | Topological persistence and dynamical heterogeneities near jamming | We introduce topological methods for quantifying spatially heterogeneous
dynamics, and use these tools to analyze particle-tracking data for a
quasi-two-dimensional granular system of air-fluidized beads on approach to
jamming. In particular we define two overlap order parameters, which quantify
the correlation betwe... | cond-mat.soft | we introduce topological methods for quantifying spatially heterogeneous dynamics and use these tools to analyze particletracking data for a quasitwodimensional granular system of airfluidized beads on approach to jamming in particular we define two overlap order parameters which quantify the correlation between partic... | [['we', 'introduce', 'topological', 'methods', 'for', 'quantifying', 'spatially', 'heterogeneous', 'dynamics', 'and', 'use', 'these', 'tools', 'to', 'analyze', 'particletracking', 'data', 'for', 'a', 'quasitwodimensional', 'granular', 'system', 'of', 'airfluidized', 'beads', 'on', 'approach', 'to', 'jamming', 'in', 'pa... | [-0.1356297740214986, 0.17730932728997592, -0.08824592405641131, 0.101550043102129, -0.033521715063473276, -0.13541227318426788, 0.03147201058454811, 0.38322655201472083, -0.24805388925918218, -0.27600293851875024, 0.08610520707804646, -0.2846133962145139, -0.16824335680857044, 0.15277983219089822, 0.015465421582861193... |
707.4179 | Inflationary perturbations in anisotropic backgrounds and their imprint
on the CMB | We extend the standard theory of cosmological perturbations to homogeneous
but anisotropic universes. We present an exhaustive computation for the case of
a Bianchi I model, with a residual isotropy between two spatial dimensions,
which is undergoing complete isotropization at the onset of inflation; we also
show how... | astro-ph gr-qc hep-ph hep-th | we extend the standard theory of cosmological perturbations to homogeneous but anisotropic universes we present an exhaustive computation for the case of a bianchi i model with a residual isotropy between two spatial dimensions which is undergoing complete isotropization at the onset of inflation we also show how the c... | [['we', 'extend', 'the', 'standard', 'theory', 'of', 'cosmological', 'perturbations', 'to', 'homogeneous', 'but', 'anisotropic', 'universes', 'we', 'present', 'an', 'exhaustive', 'computation', 'for', 'the', 'case', 'of', 'a', 'bianchi', 'i', 'model', 'with', 'a', 'residual', 'isotropy', 'between', 'two', 'spatial', 'd... | [-0.15141196075842536, 0.19128880655980462, -0.08486266508150626, 0.07556474846670357, -0.07133974344958748, -0.13147688347224085, -0.06242147613044813, 0.31458458850676774, -0.26034273323016005, -0.27317012386678274, 0.1067696827157604, -0.25479454727366, -0.12747751831609225, 0.1628722572775495, 0.016640912433509018,... |
707.418 | Oscillatory D'yakonov-Perel' spin dynamics in two dimensional electron
gases | Optical pump-probe measurements of spin-dynamics at temperatures down to 1.5K
are described for a series of (001)-oriented GaAs/AlGaAs quantum well samples
containing high mobility two-dimensional electron gases (2DEGs). For well
widths ranging from 5 nm to 20 nm and 2DEG sheet densities from 1.75x1011cm-2
to 3.5x101... | cond-mat.other | optical pumpprobe measurements of spindynamics at temperatures down to 15k are described for a series of 001oriented gaasalgaas quantum well samples containing high mobility twodimensional electron gases 2degs for well widths ranging from 5 nm to 20 nm and 2deg sheet densities from 175x1011cm2 to 35x1011cm2 the evoluti... | [['optical', 'pumpprobe', 'measurements', 'of', 'spindynamics', 'at', 'temperatures', 'down', 'to', '15k', 'are', 'described', 'for', 'a', 'series', 'of', '001oriented', 'gaasalgaas', 'quantum', 'well', 'samples', 'containing', 'high', 'mobility', 'twodimensional', 'electron', 'gases', '2degs', 'for', 'well', 'widths',... | [-0.13175056619327186, 0.23521284634156495, -0.06349535733351164, 0.04599472063320783, 0.015655509792764248, -0.1813242663684461, 0.04952478528053075, 0.36658998168371176, -0.28427638767318825, -0.31022271084097713, -0.012251367412931865, -0.32496952456174166, -0.023560342629439783, 0.23897308956545132, 0.0877393352187... |
707.4181 | Cosmological Perturbations on a Bouncing Brane | The cosmological perturbations on a bouncing brane are studied. The brane is
moving inside a Klebanov-Strassler throat where the infra-red region of the
geometry is smoothly cut off. For an observer confined to the world-volume of
the brane, this results in a non-singular bouncing mirage cosmology. We have
calculated... | hep-th astro-ph gr-qc hep-ph | the cosmological perturbations on a bouncing brane are studied the brane is moving inside a klebanovstrassler throat where the infrared region of the geometry is smoothly cut off for an observer confined to the worldvolume of the brane this results in a nonsingular bouncing mirage cosmology we have calculated the scala... | [['the', 'cosmological', 'perturbations', 'on', 'a', 'bouncing', 'brane', 'are', 'studied', 'the', 'brane', 'is', 'moving', 'inside', 'a', 'klebanovstrassler', 'throat', 'where', 'the', 'infrared', 'region', 'of', 'the', 'geometry', 'is', 'smoothly', 'cut', 'off', 'for', 'an', 'observer', 'confined', 'to', 'the', 'worl... | [-0.1576801560416214, 0.18547865021168508, -0.1430140159828546, 0.08354764992369075, -0.07593692129915877, -0.12850310579346297, -0.042696345617971275, 0.30973736185699563, -0.20564788097800626, -0.248827230508469, 0.10029048477320775, -0.27423129066586766, -0.053166291227810865, 0.12753935069160444, -0.053237966252368... |
707.4182 | A Luminosity Function of Lyman Alpha Emitting Galaxies at Redshift 4.5 | We present a catalog of 59 z=4.5 Lyman alpha emitting galaxies
spectroscopically confirmed in a campaign of Keck/DEIMOS follow-up observations
to candidates selected in the Large Area Lyman Alpha (LALA) narrow-band imaging
survey. We targeted 97 candidates for spectroscopic follow-up; by accounting
for the variety of... | astro-ph | we present a catalog of 59 z45 lyman alpha emitting galaxies spectroscopically confirmed in a campaign of keckdeimos followup observations to candidates selected in the large area lyman alpha lala narrowband imaging survey we targeted 97 candidates for spectroscopic followup by accounting for the variety of conditions ... | [['we', 'present', 'a', 'catalog', 'of', '59', 'z45', 'lyman', 'alpha', 'emitting', 'galaxies', 'spectroscopically', 'confirmed', 'in', 'a', 'campaign', 'of', 'keckdeimos', 'followup', 'observations', 'to', 'candidates', 'selected', 'in', 'the', 'large', 'area', 'lyman', 'alpha', 'lala', 'narrowband', 'imaging', 'surve... | [-0.03772390271478798, 0.08838142460444942, -0.015389479072688178, 0.09188048904150968, -0.05678553686412357, -0.09613344792971296, 0.14902329509486215, 0.45637233653411147, -0.05527151980414437, -0.40294146580148305, 0.00691917019181257, -0.35817792684939065, 0.00712135668197975, 0.1809472625390016, 0.0568168224637076... |
707.4183 | Electric Charge in Interaction with Magnetically Charged Black Holes | We examine the angular momentum of an electric charge e placed at rest
outside a dilaton black hole with magnetic charge Q. The electromagnetic
angular momentum which is stored in the electromagnetic field outside the black
hole shows several common features regardless of the dilaton coupling strength,
though the dil... | gr-qc | we examine the angular momentum of an electric charge e placed at rest outside a dilaton black hole with magnetic charge q the electromagnetic angular momentum which is stored in the electromagnetic field outside the black hole shows several common features regardless of the dilaton coupling strength though the dilaton... | [['we', 'examine', 'the', 'angular', 'momentum', 'of', 'an', 'electric', 'charge', 'e', 'placed', 'at', 'rest', 'outside', 'a', 'dilaton', 'black', 'hole', 'with', 'magnetic', 'charge', 'q', 'the', 'electromagnetic', 'angular', 'momentum', 'which', 'is', 'stored', 'in', 'the', 'electromagnetic', 'field', 'outside', 'th... | [-0.15829238710466598, 0.15096887927764632, -0.04404110619361745, 0.13124533752003723, -0.07318741729250178, -0.14753745406293697, 0.005352441533129119, 0.3269683555748391, -0.20132082054624334, -0.3291373232417148, 0.050455924630417336, -0.32500892055880587, -0.06426062793616438, 0.18275703972904012, -0.03663990092657... |
707.4184 | Restriction of characters and products of characters | Let G be a finite p-group, for some prime p, and $\psi, \theta \in \Irr(G)$
be irreducible complex characters of G. It has been proved that if, in
addition, $\psi,\theta$ are faithful characters, then the product $\psi\theta$
is a multiple of an irreducible or it is the nontrivial linear combination of
at least $\fra... | math.GR | let g be a finite pgroup for some prime p and psi theta in irrg be irreducible complex characters of g it has been proved that if in addition psitheta are faithful characters then the product psitheta is a multiple of an irreducible or it is the nontrivial linear combination of at least fracp12 distinct irreducible cha... | [['let', 'g', 'be', 'a', 'finite', 'pgroup', 'for', 'some', 'prime', 'p', 'and', 'psi', 'theta', 'in', 'irrg', 'be', 'irreducible', 'complex', 'characters', 'of', 'g', 'it', 'has', 'been', 'proved', 'that', 'if', 'in', 'addition', 'psitheta', 'are', 'faithful', 'characters', 'then', 'the', 'product', 'psitheta', 'is', ... | [-0.20304600652095608, 0.15356572700507096, -0.15399943564995383, -0.008537223860852358, -0.13687312468301413, -0.153378249065227, -0.03928729411876522, 0.3810294624379536, -0.3342640625143593, -0.2081201074198504, 0.07594172851459607, -0.2847053326420055, -0.1378286115167093, 0.17563568261521292, -0.07178096385087726,... |
707.4185 | Frozen fronts in cellular flows | We present experiments on the behavior of reaction fronts in ordered and
disordered cellular flows with imposed winds. Fronts in a chain of alternating
vortices are found to freeze (pin to the separatrix) for a wide range of
imposed winds that grows nonlinearly with the characteristic strength of the
underlying vorti... | nlin.PS | we present experiments on the behavior of reaction fronts in ordered and disordered cellular flows with imposed winds fronts in a chain of alternating vortices are found to freeze pin to the separatrix for a wide range of imposed winds that grows nonlinearly with the characteristic strength of the underlying vorticity ... | [['we', 'present', 'experiments', 'on', 'the', 'behavior', 'of', 'reaction', 'fronts', 'in', 'ordered', 'and', 'disordered', 'cellular', 'flows', 'with', 'imposed', 'winds', 'fronts', 'in', 'a', 'chain', 'of', 'alternating', 'vortices', 'are', 'found', 'to', 'freeze', 'pin', 'to', 'the', 'separatrix', 'for', 'a', 'wide... | [-0.208354068454355, 0.21827735248303345, -0.04780452089082331, 0.029951390044135582, -0.060883807730427834, -0.09917380756611914, 0.02075095120330103, 0.38841855128533964, -0.3042953009608873, -0.20040518977830923, 0.0946323599146549, -0.2408557959702299, -0.14499880756836298, 0.22498661396635133, 0.001978176201931959... |
707.4186 | Derivative Dispersion Relations for the Amplitude Slopes in pp and
p-pbar Scattering | We extend the use of derivative dispersion relations to the study of slopes
of the real and imaginary amplitudes in pp and p-pbar elastic scattering. The
new relations are tested against the solutions for the amplitudes obtained in
the analysis of the high energy data. Extensions beyond the forward direction
are inve... | hep-ph | we extend the use of derivative dispersion relations to the study of slopes of the real and imaginary amplitudes in pp and ppbar elastic scattering the new relations are tested against the solutions for the amplitudes obtained in the analysis of the high energy data extensions beyond the forward direction are investiga... | [['we', 'extend', 'the', 'use', 'of', 'derivative', 'dispersion', 'relations', 'to', 'the', 'study', 'of', 'slopes', 'of', 'the', 'real', 'and', 'imaginary', 'amplitudes', 'in', 'pp', 'and', 'ppbar', 'elastic', 'scattering', 'the', 'new', 'relations', 'are', 'tested', 'against', 'the', 'solutions', 'for', 'the', 'ampli... | [-0.1356663010083139, 0.1012165394360916, -0.11222709793946706, 0.14911379905131, -0.05867639201908158, -0.0447322830486183, 0.01716925575433729, 0.32914435180674234, -0.24026231600258213, -0.2544002978919217, 0.06335299698940407, -0.34668948436872316, -0.080376964671394, 0.21755288111475798, 0.05969179102864403, 0.101... |
707.4187 | Is Small Perfect? Size Limit to Defect Formation in Pyramidal Pt
Nanocontacts | We report high resolution transmission electron microscopy and ab initio
calculation results for the defect formation in Pt nanocontacts (NCs). Our
results show that there is a size limit to the existence of twins (extended
structural defects). Defects are always present but blocked away from the tip
axes. The twins ... | cond-mat.mtrl-sci | we report high resolution transmission electron microscopy and ab initio calculation results for the defect formation in pt nanocontacts ncs our results show that there is a size limit to the existence of twins extended structural defects defects are always present but blocked away from the tip axes the twins may act a... | [['we', 'report', 'high', 'resolution', 'transmission', 'electron', 'microscopy', 'and', 'ab', 'initio', 'calculation', 'results', 'for', 'the', 'defect', 'formation', 'in', 'pt', 'nanocontacts', 'ncs', 'our', 'results', 'show', 'that', 'there', 'is', 'a', 'size', 'limit', 'to', 'the', 'existence', 'of', 'twins', 'exte... | [-0.15006718335633862, 0.16978405191379428, -0.052916883353248866, 0.0097110237627828, 0.03141060265266454, -0.1546986139458145, 0.10191376542288837, 0.45993625417246786, -0.22561780499740386, -0.31085250033459194, 0.02870815323213194, -0.3503801430719839, -0.11057522875899581, 0.15467215212337462, 0.017377116396026293... |
707.4188 | Well-posed initial-boundary value problem for the harmonic Einstein
equations using energy estimates | In recent work, we used pseudo-differential theory to establish conditions
that the initial-boundary value problem for second order systems of wave
equations be strongly well-posed in a generalized sense. The applications
included the harmonic version of the Einstein equations. Here we show that
these results can als... | gr-qc | in recent work we used pseudodifferential theory to establish conditions that the initialboundary value problem for second order systems of wave equations be strongly wellposed in a generalized sense the applications included the harmonic version of the einstein equations here we show that these results can also be obt... | [['in', 'recent', 'work', 'we', 'used', 'pseudodifferential', 'theory', 'to', 'establish', 'conditions', 'that', 'the', 'initialboundary', 'value', 'problem', 'for', 'second', 'order', 'systems', 'of', 'wave', 'equations', 'be', 'strongly', 'wellposed', 'in', 'a', 'generalized', 'sense', 'the', 'applications', 'include... | [-0.11698382564425243, 0.05093233381172247, -0.06572335304438391, 0.10055972921492701, -0.08157646539973828, -0.08808288255452433, -0.046061214915067525, 0.28086089976414136, -0.3084809452958518, -0.2294355652323275, 0.143472587037126, -0.23772337173365735, -0.19133661323311654, 0.23507420680570332, -0.066112451798593,... |
707.4189 | Superfluid-Insulator Transition and Fermion Pairing in Bose-Fermi
Mixtures | It is well known that bosons on an optical lattice undergo a second-order
superfluid-insulator transition (SIT) when the lattice potential increases. In
this paper we study SIT when fermions coexist with the bosons. We find that the
critical properties of particle-hole symmetric SIT with dynamical exponent z=1
is mod... | cond-mat.supr-con cond-mat.str-el | it is well known that bosons on an optical lattice undergo a secondorder superfluidinsulator transition sit when the lattice potential increases in this paper we study sit when fermions coexist with the bosons we find that the critical properties of particlehole symmetric sit with dynamical exponent z1 is modified when... | [['it', 'is', 'well', 'known', 'that', 'bosons', 'on', 'an', 'optical', 'lattice', 'undergo', 'a', 'secondorder', 'superfluidinsulator', 'transition', 'sit', 'when', 'the', 'lattice', 'potential', 'increases', 'in', 'this', 'paper', 'we', 'study', 'sit', 'when', 'fermions', 'coexist', 'with', 'the', 'bosons', 'we', 'fi... | [-0.17710700521259853, 0.31360807306532945, -0.05408575685875376, 0.05882534016237347, -0.030933778213303804, -0.25502827039525405, 0.056878739964378505, 0.3714707183879705, -0.19576474856015066, -0.18130718899548662, 0.037860487508159894, -0.3635484914067296, -0.20472348449343092, 0.09409951324318061, 0.10004069408097... |
707.419 | PAH Emission from Ultraluminous Infrared Galaxies | We explore the relationships between the Polycyclic Aromatic Hydrocarbon
(PAH) feature strengths, mid-infrared continuum luminosities, far-infrared
spectral slopes, optical spectroscopic classifications, and silicate optical
depths within a sample of 107 ULIRGs observed with the Infrared Spectrograph on
the Spitzer S... | astro-ph | we explore the relationships between the polycyclic aromatic hydrocarbon pah feature strengths midinfrared continuum luminosities farinfrared spectral slopes optical spectroscopic classifications and silicate optical depths within a sample of 107 ulirgs observed with the infrared spectrograph on the spitzer space teles... | [['we', 'explore', 'the', 'relationships', 'between', 'the', 'polycyclic', 'aromatic', 'hydrocarbon', 'pah', 'feature', 'strengths', 'midinfrared', 'continuum', 'luminosities', 'farinfrared', 'spectral', 'slopes', 'optical', 'spectroscopic', 'classifications', 'and', 'silicate', 'optical', 'depths', 'within', 'a', 'sam... | [0.033188148244770004, 0.11608272518492742, -0.02562061958194931, 0.10901507426892376, -0.006213664499016992, -0.09825800002242129, 0.006777098537074033, 0.5939256211445816, -0.093410987160641, -0.32389655342811474, -0.020020237935291927, -0.3264588023408525, 0.028259409029162737, 0.12295057077635603, -0.03081082721136... |
707.4191 | Neutron Form Factor from Neutrino-Nucleus Coherent Elastic Scattering | We analyze the prospect of measuring the neutron form factor of a nucleus
through the detection of neutrino-nucleus coherent elastic scattering. We
predict numbers of events in a liquid noble nuclear recoil detector at a
stopped pion neutrino source. We discuss the precision required to distinguish
between different ... | hep-ph nucl-th | we analyze the prospect of measuring the neutron form factor of a nucleus through the detection of neutrinonucleus coherent elastic scattering we predict numbers of events in a liquid noble nuclear recoil detector at a stopped pion neutrino source we discuss the precision required to distinguish between different theor... | [['we', 'analyze', 'the', 'prospect', 'of', 'measuring', 'the', 'neutron', 'form', 'factor', 'of', 'a', 'nucleus', 'through', 'the', 'detection', 'of', 'neutrinonucleus', 'coherent', 'elastic', 'scattering', 'we', 'predict', 'numbers', 'of', 'events', 'in', 'a', 'liquid', 'noble', 'nuclear', 'recoil', 'detector', 'at',... | [-0.07482113481361281, 0.21444578908590806, -0.08545635187894934, 0.1567020770162344, -0.0009752293462278667, -0.06672639178146643, 0.0954203807093479, 0.3455380170985504, -0.24585108661644714, -0.2921045955132555, -0.03597240237501898, -0.3509108277762102, -0.018290966654334356, 0.1885506042443147, 0.08499949350435701... |
707.4192 | Improved Lewenstein model for high-order harmonic generation of atoms
and molecules with scattering wavefunctions | We demonstrate a simple method to improve the Lewenstein model for the
description of high-order harmonic generation (HHG). It is shown that HHG
spectra can be expressed as the product of a returning electron wave packet and
the photo-recombination cross sections, where the former can be extracted from
the Lewenstein... | physics.atom-ph | we demonstrate a simple method to improve the lewenstein model for the description of highorder harmonic generation hhg it is shown that hhg spectra can be expressed as the product of a returning electron wave packet and the photorecombination cross sections where the former can be extracted from the lewenstein model b... | [['we', 'demonstrate', 'a', 'simple', 'method', 'to', 'improve', 'the', 'lewenstein', 'model', 'for', 'the', 'description', 'of', 'highorder', 'harmonic', 'generation', 'hhg', 'it', 'is', 'shown', 'that', 'hhg', 'spectra', 'can', 'be', 'expressed', 'as', 'the', 'product', 'of', 'a', 'returning', 'electron', 'wave', 'pa... | [-0.03356726165289616, 0.13670240988302015, -0.07166735292172309, 0.05263368617479219, 0.006154345334075468, -0.07998151661463312, -0.03699301441497717, 0.38052001333382635, -0.268790384826548, -0.27071925113457684, -0.0025134434810714775, -0.31908367136397314, -0.12484908228519268, 0.2437146841212339, 0.04815789941967... |
707.4193 | On the interaction of Jupiter's Great Red Spot and zonal jet streams | In this paper, Jupiter's Great Red Spot (GRS) is used to determine properties
of the Jovian atmosphere that cannot otherwise be found. These properties
include the potential vorticity of the GRS and its neighboring jet streams, the
shear imposed on the GRS by the jet streams, and the vertical entropy gradient
(i.e., ... | physics.flu-dyn physics.ao-ph | in this paper jupiters great red spot grs is used to determine properties of the jovian atmosphere that cannot otherwise be found these properties include the potential vorticity of the grs and its neighboring jet streams the shear imposed on the grs by the jet streams and the vertical entropy gradient ie rossby deform... | [['in', 'this', 'paper', 'jupiters', 'great', 'red', 'spot', 'grs', 'is', 'used', 'to', 'determine', 'properties', 'of', 'the', 'jovian', 'atmosphere', 'that', 'can', 'not', 'otherwise', 'be', 'found', 'these', 'properties', 'include', 'the', 'potential', 'vorticity', 'of', 'the', 'grs', 'and', 'its', 'neighboring', 'j... | [-0.16779144621990927, 0.10462601831496025, -0.09354289638319473, 0.06632849767565134, -0.1083318259262076, -0.0692947815497925, 0.001753768202152301, 0.3368663336995132, -0.27091442572521623, -0.2952387594716805, 0.14549022870070294, -0.25742957375807674, -0.0739094609594533, 0.16867120197636232, -0.058651940916295046... |
707.4194 | Tests of non-standard electroweak couplings of right-handed quarks | The standard model can be interpreted as the leading order of a Low-Energy
Effective Theory (LEET) invariant under a higher non linearly realized symmetry
$S_{nat}\supset SU(2)_W \times U(1)_Y$ equipped with a systematic power
counting. Within the minimal version of this ``not quite decoupling'' LEET, the
dominant no... | hep-ph hep-ex | the standard model can be interpreted as the leading order of a lowenergy effective theory leet invariant under a higher non linearly realized symmetry s_natsupset su2_w times u1_y equipped with a systematic power counting within the minimal version of this not quite decoupling leet the dominant nonstandard effect appe... | [['the', 'standard', 'model', 'can', 'be', 'interpreted', 'as', 'the', 'leading', 'order', 'of', 'a', 'lowenergy', 'effective', 'theory', 'leet', 'invariant', 'under', 'a', 'higher', 'non', 'linearly', 'realized', 'symmetry', 's_natsupset', 'su2_w', 'times', 'u1_y', 'equipped', 'with', 'a', 'systematic', 'power', 'coun... | [-0.14393634910246345, 0.2900390013904359, -0.04481308301240742, 0.146705060975338, -0.0845769721203946, -0.17244225150148432, 0.028468948272190882, 0.30904660874093287, -0.2002226134105552, -0.2649083647629072, 0.008621319007001174, -0.28995845175395124, -0.00012810238831334836, 0.07750521406444232, 0.0401689390561429... |
707.4195 | Experiments with Probabilistic Quantum Auctions | We describe human-subject laboratory experiments on probabilistic auctions
based on previously proposed auction protocols involving the simulated
manipulation and communication of quantum states. These auctions are
probabilistic in determining which bidder wins, or having no winner, rather
than always having the high... | quant-ph | we describe humansubject laboratory experiments on probabilistic auctions based on previously proposed auction protocols involving the simulated manipulation and communication of quantum states these auctions are probabilistic in determining which bidder wins or having no winner rather than always having the highest bi... | [['we', 'describe', 'humansubject', 'laboratory', 'experiments', 'on', 'probabilistic', 'auctions', 'based', 'on', 'previously', 'proposed', 'auction', 'protocols', 'involving', 'the', 'simulated', 'manipulation', 'and', 'communication', 'of', 'quantum', 'states', 'these', 'auctions', 'are', 'probabilistic', 'in', 'det... | [-0.10388901043812179, 0.02575060467331371, -0.08786968322653722, 0.10738363435042889, -0.10894326927206878, -0.29349849906118053, 0.16254253953957232, 0.4346201975796638, -0.23349388090926887, -0.3121427070044384, 0.05953394108759572, -0.28412469115573913, -0.1284157389059796, 0.21037859736991646, -0.1213827560880288,... |
707.4196 | A short Brownian motion proof of the Riemann hypothesis | We give a short probabilistic (a Brownian motion) proof of the Riemann
hypothesis based on some surprising, unexpected and deep algebraic conjecture
(MAC in short) concerning the relation between the Riemann zeta $\xi$ and a
trivial zeta $\zeta_{t}$. That algebraic conjecture was firstly discovered and
formulated in ... | math.GM | we give a short probabilistic a brownian motion proof of the riemann hypothesis based on some surprising unexpected and deep algebraic conjecture mac in short concerning the relation between the riemann zeta xi and a trivial zeta zeta_t that algebraic conjecture was firstly discovered and formulated in ma | [['we', 'give', 'a', 'short', 'probabilistic', 'a', 'brownian', 'motion', 'proof', 'of', 'the', 'riemann', 'hypothesis', 'based', 'on', 'some', 'surprising', 'unexpected', 'and', 'deep', 'algebraic', 'conjecture', 'mac', 'in', 'short', 'concerning', 'the', 'relation', 'between', 'the', 'riemann', 'zeta', 'xi', 'and', '... | [-0.27803737912715104, 0.0676870962488465, -0.2108273554670935, 0.1453308670509917, -0.12246978122857399, -0.21386498495121486, 0.07191502236916374, 0.2856171589034299, -0.27939090862249333, -0.23519600473809987, 0.05483646787373194, -0.1594143881520722, -0.2315003440792983, 0.20447786641307175, -0.10266636108281091, 0... |
707.4197 | Ascent of module structures, vanishing of Ext, and extended modules | Let $(R,\m)$ and $(S,\n)$ be commutative Noetherian local rings, and let
$\phi:R\to S$ be a flat local homomorphism such that $\m S = \n$ and the
induced map on residue fields $R/\m \to S/\n$ is an isomorphism. Given a
finitely generated $R$-module $M$, we show that $M$ has an $S$-module structure
compatible with the... | math.AC | let rm and sn be commutative noetherian local rings and let phirto s be a flat local homomorphism such that m s n and the induced map on residue fields rm to sn is an isomorphism given a finitely generated rmodule m we show that m has an smodule structure compatible with the given rmodule structure if and only if exti_... | [['let', 'rm', 'and', 'sn', 'be', 'commutative', 'noetherian', 'local', 'rings', 'and', 'let', 'phirto', 's', 'be', 'a', 'flat', 'local', 'homomorphism', 'such', 'that', 'm', 's', 'n', 'and', 'the', 'induced', 'map', 'on', 'residue', 'fields', 'rm', 'to', 'sn', 'is', 'an', 'isomorphism', 'given', 'a', 'finitely', 'gene... | [-0.18917898365341695, 0.11175680795349763, -0.0667989746046563, 0.021227259205059253, -0.04113657477460543, -0.2118061012685454, -0.09427021820172538, 0.40150829567573965, -0.4124033856852394, -0.17362833764552002, 0.0937234765668917, -0.25170263905440354, -0.08933738178812847, 0.18559168652993524, -0.0879045416691547... |
707.4198 | Reductionism, emergence, and levels of abstractions | Can there be independent higher level laws of nature if everything is
reducible to the fundamental laws of physics? The computer science notion of
level of abstraction explains why there can -- illustrating how computational
thinking can solve one of philosophy's most vexing problems.
| cs.OH | can there be independent higher level laws of nature if everything is reducible to the fundamental laws of physics the computer science notion of level of abstraction explains why there can illustrating how computational thinking can solve one of philosophys most vexing problems | [['can', 'there', 'be', 'independent', 'higher', 'level', 'laws', 'of', 'nature', 'if', 'everything', 'is', 'reducible', 'to', 'the', 'fundamental', 'laws', 'of', 'physics', 'the', 'computer', 'science', 'notion', 'of', 'level', 'of', 'abstraction', 'explains', 'why', 'there', 'can', 'illustrating', 'how', 'computation... | [-0.0861516370925875, 0.1578463865887551, -0.12483069114387035, 0.12280555376838449, -0.15478984655124978, -0.21147754154212417, 0.011889272724233922, 0.25729069287522827, -0.3695343831648296, -0.38313510548323393, 0.06439189790260225, -0.21246106354963212, -0.21155121567703428, 0.22391198916981617, -0.1650942105001636... |
707.4199 | On the Possibility of the Detection of Extinct Radio Pulsars | We explore the possibilities for detecting pulsars that have ceased to
radiate in the radio band. We consider two models: the model with hindered
particle escape from the pulsar surface (first suggested by Ruderman and
Sutherland 1975) and the model with free particle escape (Arons 1981; Mestel
1999). In the model wi... | astro-ph | we explore the possibilities for detecting pulsars that have ceased to radiate in the radio band we consider two models the model with hindered particle escape from the pulsar surface first suggested by ruderman and sutherland 1975 and the model with free particle escape arons 1981 mestel 1999 in the model with hindere... | [['we', 'explore', 'the', 'possibilities', 'for', 'detecting', 'pulsars', 'that', 'have', 'ceased', 'to', 'radiate', 'in', 'the', 'radio', 'band', 'we', 'consider', 'two', 'models', 'the', 'model', 'with', 'hindered', 'particle', 'escape', 'from', 'the', 'pulsar', 'surface', 'first', 'suggested', 'by', 'ruderman', 'and... | [-0.05169791875120539, 0.24015920100590357, -0.03127612989718238, 0.12587984600641694, -0.11160378987685993, -0.14121235077484295, 0.039917262457311156, 0.39632492400705815, -0.22552582136928462, -0.38011529710000524, 0.07202083579569052, -0.3144595022671498, -0.033097225370315404, 0.2499013535785847, -0.02162958443021... |
707.42 | QCD Corrections to QED Vacuum Polarization | We compute QCD corrections to QED calculations for vacuum polarization in
background magnetic fields. Formally, the diagram for virtual $e\bar{e}$ loops
is identical to the one for virtual $q\bar{q}$ loops. However due to
confinement, or to the growth of $\alpha_s$ as $p^2$ decreases, a direct
calculation of the diag... | hep-ph | we compute qcd corrections to qed calculations for vacuum polarization in background magnetic fields formally the diagram for virtual ebare loops is identical to the one for virtual qbarq loops however due to confinement or to the growth of alpha_s as p2 decreases a direct calculation of the diagram is not allowed at l... | [['we', 'compute', 'qcd', 'corrections', 'to', 'qed', 'calculations', 'for', 'vacuum', 'polarization', 'in', 'background', 'magnetic', 'fields', 'formally', 'the', 'diagram', 'for', 'virtual', 'ebare', 'loops', 'is', 'identical', 'to', 'the', 'one', 'for', 'virtual', 'qbarq', 'loops', 'however', 'due', 'to', 'confineme... | [-0.10635148362470333, 0.268792879874589, -0.035812432002377964, 0.14629384693788247, -0.031888623008138085, -0.09968179690554901, 0.05768467754614158, 0.37577320962808414, -0.18766727395192848, -0.26554046177478313, -0.009855278828715692, -0.3253143041857768, 0.011299588255675846, 0.16519252434271117, 0.07563319079729... |
707.4201 | Noncommutative geometry and lower dimensional volumes in Riemannian
geometry | In this paper we explain how to define "lower dimensional'' volumes of any
compact Riemannian manifold as the integrals of local Riemannian invariants.
For instance we give sense to the area and the length of such a manifold in any
dimension. Our reasoning is motivated by an idea of Connes and involves in an
essentia... | math.DG math.OA | in this paper we explain how to define lower dimensional volumes of any compact riemannian manifold as the integrals of local riemannian invariants for instance we give sense to the area and the length of such a manifold in any dimension our reasoning is motivated by an idea of connes and involves in an essential way n... | [['in', 'this', 'paper', 'we', 'explain', 'how', 'to', 'define', 'lower', 'dimensional', 'volumes', 'of', 'any', 'compact', 'riemannian', 'manifold', 'as', 'the', 'integrals', 'of', 'local', 'riemannian', 'invariants', 'for', 'instance', 'we', 'give', 'sense', 'to', 'the', 'area', 'and', 'the', 'length', 'of', 'such', ... | [-0.13247334469821961, 0.10121511538985514, -0.0684101078330594, 0.11245734462624087, -0.09151417031500708, -0.09450208605541026, -0.02034038609742899, 0.3240059317473103, -0.253219030446866, -0.283946379975361, 0.1103386921054848, -0.2439301044899313, -0.18545019419809036, 0.21110789519186843, -0.1545729287680896, 0.0... |
707.4202 | Multiclass Hammersley-Aldous-Diaconis process and multiclass-customer
queues | In the Hammersley-Aldous-Diaconis process infinitely many particles sit in R
and at most one particle is allowed at each position. A particle at x$ whose
nearest neighbor to the right is at y, jumps at rate y-x to a position
uniformly distributed in the interval (x,y). The basic coupling between
trajectories with dif... | math.PR math-ph math.MP | in the hammersleyaldousdiaconis process infinitely many particles sit in r and at most one particle is allowed at each position a particle at x whose nearest neighbor to the right is at y jumps at rate yx to a position uniformly distributed in the interval xy the basic coupling between trajectories with different initi... | [['in', 'the', 'hammersleyaldousdiaconis', 'process', 'infinitely', 'many', 'particles', 'sit', 'in', 'r', 'and', 'at', 'most', 'one', 'particle', 'is', 'allowed', 'at', 'each', 'position', 'a', 'particle', 'at', 'x', 'whose', 'nearest', 'neighbor', 'to', 'the', 'right', 'is', 'at', 'y', 'jumps', 'at', 'rate', 'yx', 't... | [-0.12740439797296774, 0.14520545148312353, -0.07393915115985586, 0.033139175251681294, -0.009175390126400215, -0.16891663994336892, 0.05980313872041311, 0.3511669598693071, -0.31507678188784266, -0.24908386095925125, 0.08273063614412189, -0.28305232623202164, -0.0667051350308019, 0.12383907668963941, -0.01187805071213... |
707.4203 | Uniform Uncertainty Principle and signal recovery via Regularized
Orthogonal Matching Pursuit | This paper seeks to bridge the two major algorithmic approaches to sparse
signal recovery from an incomplete set of linear measurements --
L_1-minimization methods and iterative methods (Matching Pursuits). We find a
simple regularized version of the Orthogonal Matching Pursuit (ROMP) which has
advantages of both app... | math.NA | this paper seeks to bridge the two major algorithmic approaches to sparse signal recovery from an incomplete set of linear measurements l_1minimization methods and iterative methods matching pursuits we find a simple regularized version of the orthogonal matching pursuit romp which has advantages of both approaches the... | [['this', 'paper', 'seeks', 'to', 'bridge', 'the', 'two', 'major', 'algorithmic', 'approaches', 'to', 'sparse', 'signal', 'recovery', 'from', 'an', 'incomplete', 'set', 'of', 'linear', 'measurements', 'l_1minimization', 'methods', 'and', 'iterative', 'methods', 'matching', 'pursuits', 'we', 'find', 'a', 'simple', 'regu... | [-0.1043876687441259, -0.016414164529433426, -0.11700262650451128, 0.0408838934839723, -0.09428961100205382, -0.13547350301288386, 0.056465174064369614, 0.3888037302630379, -0.3196714040724204, -0.2660370321122018, 0.12865948591980728, -0.25767264423020025, -0.16947719855159718, 0.1360721978621478, -0.1161579847474523,... |
707.4204 | Double bracket dissipation in kinetic theory for particles with
anisotropic interactions | We derive equations of motion for the dynamics of anisotropic particles
directly from the dissipative Vlasov kinetic equations, with the dissipation
given by the double bracket approach (Double Bracket Vlasov, or DBV). The
moments of the DBV equation lead to a nonlocal form of Darcy's law for the mass
density. Next, ... | nlin.AO cond-mat.mes-hall nlin.PS physics.chem-ph | we derive equations of motion for the dynamics of anisotropic particles directly from the dissipative vlasov kinetic equations with the dissipation given by the double bracket approach double bracket vlasov or dbv the moments of the dbv equation lead to a nonlocal form of darcys law for the mass density next kinetic eq... | [['we', 'derive', 'equations', 'of', 'motion', 'for', 'the', 'dynamics', 'of', 'anisotropic', 'particles', 'directly', 'from', 'the', 'dissipative', 'vlasov', 'kinetic', 'equations', 'with', 'the', 'dissipation', 'given', 'by', 'the', 'double', 'bracket', 'approach', 'double', 'bracket', 'vlasov', 'or', 'dbv', 'the', '... | [-0.1117401390445919, 0.12207620005721032, -0.10238863366530902, 0.101953008546626, -0.0912121308258554, -0.128572533800225, -0.04145533834330376, 0.2504893474058429, -0.2989818936321579, -0.31387391641958434, 0.005771463656964809, -0.2270184739548435, -0.11286753550373407, 0.19436983268363958, 0.03015385029503881, 0.0... |
707.4205 | Symbolic Models for Nonlinear Control Systems: Alternating Approximate
Bisimulations | Symbolic models are abstract descriptions of continuous systems in which
symbols represent aggregates of continuous states. In the last few years there
has been a growing interest in the use of symbolic models as a tool for
mitigating complexity in control design. In fact, symbolic models enable the
use of well known... | math.OC | symbolic models are abstract descriptions of continuous systems in which symbols represent aggregates of continuous states in the last few years there has been a growing interest in the use of symbolic models as a tool for mitigating complexity in control design in fact symbolic models enable the use of well known algo... | [['symbolic', 'models', 'are', 'abstract', 'descriptions', 'of', 'continuous', 'systems', 'in', 'which', 'symbols', 'represent', 'aggregates', 'of', 'continuous', 'states', 'in', 'the', 'last', 'few', 'years', 'there', 'has', 'been', 'a', 'growing', 'interest', 'in', 'the', 'use', 'of', 'symbolic', 'models', 'as', 'a',... | [-0.09932354546781681, 0.06949083921893066, -0.07183065124406991, 0.04735347508980801, -0.05871493524124085, -0.16351097275283266, -0.007805804954841733, 0.37520783859724016, -0.30112711634014694, -0.2916783543539719, 0.16406571741533976, -0.22245903039665918, -0.21888667589027277, 0.2643898787422919, -0.13494418745755... |
707.4206 | Interferometry of non-Abelian Anyons | We develop the general quantum measurement theory of non-Abelian anyons
through interference experiments. The paper starts with a terse introduction to
the theory of anyon models, focusing on the basic formalism necessary to apply
standard quantum measurement theory to such systems. This is then applied to
give a det... | quant-ph cond-mat.mes-hall hep-th | we develop the general quantum measurement theory of nonabelian anyons through interference experiments the paper starts with a terse introduction to the theory of anyon models focusing on the basic formalism necessary to apply standard quantum measurement theory to such systems this is then applied to give a detailed ... | [['we', 'develop', 'the', 'general', 'quantum', 'measurement', 'theory', 'of', 'nonabelian', 'anyons', 'through', 'interference', 'experiments', 'the', 'paper', 'starts', 'with', 'a', 'terse', 'introduction', 'to', 'the', 'theory', 'of', 'anyon', 'models', 'focusing', 'on', 'the', 'basic', 'formalism', 'necessary', 'to... | [-0.138078352702047, 0.19704056220094154, -0.10780720643812852, 0.09006392409229222, -0.0305293164797512, -0.19543542548305762, 0.07736678860705573, 0.3233816079498037, -0.1999403816984503, -0.3191794749207116, 0.03666779272938191, -0.2760335068270879, -0.12730119617638383, 0.19428290560089506, -0.013893864745139735, 0... |
707.4207 | Large time asymptotics of growth models on space-like paths II: PNG and
parallel TASEP | We consider the polynuclear growth (PNG) model in 1+1 dimension with flat
initial condition and no extra constraints. The joint distributions of surface
height at finitely many points at a fixed time moment are given as marginals of
a signed determinantal point process. The long time scaling limit of the
surface heig... | math-ph cond-mat.stat-mech math.MP math.PR | we consider the polynuclear growth png model in 11 dimension with flat initial condition and no extra constraints the joint distributions of surface height at finitely many points at a fixed time moment are given as marginals of a signed determinantal point process the long time scaling limit of the surface height is s... | [['we', 'consider', 'the', 'polynuclear', 'growth', 'png', 'model', 'in', '11', 'dimension', 'with', 'flat', 'initial', 'condition', 'and', 'no', 'extra', 'constraints', 'the', 'joint', 'distributions', 'of', 'surface', 'height', 'at', 'finitely', 'many', 'points', 'at', 'a', 'fixed', 'time', 'moment', 'are', 'given', ... | [-0.14811757521118163, 0.13589332117243028, -0.0972931653779653, 0.07708502005869039, -0.0426973858680192, -0.16041189929489622, 0.04851064863962784, 0.3817988782016964, -0.2694835515174362, -0.23085579950453655, 0.09886260499899305, -0.24247105732636967, -0.07891167393050243, 0.18837493379389117, -0.021667697097261233... |
707.4208 | Research News -- Observation of Exotic Heavy Baryons | We review the recent discoveries of exotic heavy baryons at the Fermi
National Accelerator Laboratory.
| physics.pop-ph hep-ex hep-ph | we review the recent discoveries of exotic heavy baryons at the fermi national accelerator laboratory | [['we', 'review', 'the', 'recent', 'discoveries', 'of', 'exotic', 'heavy', 'baryons', 'at', 'the', 'fermi', 'national', 'accelerator', 'laboratory']] | [-0.1122316108395656, 0.31029918485631547, -0.10143664767965674, 0.12884691700649759, -0.08921907618641853, -0.13780243024230004, 0.07140238881111145, 0.2036535732448101, -0.1660803636536002, -0.334908094505469, -0.08203769751513998, -0.4732920224467913, 0.06999871879816055, 0.23431756955881913, 0.09281884624312321, 0.... |
707.4209 | Research News -- Observation of oscillation phenomena in heavy meson
systems | We review the recent discoveries of rare oscillation phenomena in certain
heavy neutral meson systems.
| physics.pop-ph hep-ex hep-ph | we review the recent discoveries of rare oscillation phenomena in certain heavy neutral meson systems | [['we', 'review', 'the', 'recent', 'discoveries', 'of', 'rare', 'oscillation', 'phenomena', 'in', 'certain', 'heavy', 'neutral', 'meson', 'systems']] | [-0.2052004654891789, 0.3587701287741462, 0.015326153486967087, 0.1538756822546323, -0.05786979744831721, -0.14829894949992498, 0.12030490823090076, 0.20516769948105018, -0.21713474448770284, -0.1959689274430275, -0.0040182117450361455, -0.40391461650530497, -0.16218379512429237, 0.1631826963275671, 0.00594222284853458... |
707.421 | Sampling Lissajous and Fourier knots | A Lissajous knot is one that can be parameterized by a single cosine function
in each coordinate. Lissajous knots are highly symmetric, and for this reason,
not all knots are Lissajous. We prove several theorems which allow us to place
bounds on the number of Lissajous knot types with given frequencies and to
efficie... | math.GT | a lissajous knot is one that can be parameterized by a single cosine function in each coordinate lissajous knots are highly symmetric and for this reason not all knots are lissajous we prove several theorems which allow us to place bounds on the number of lissajous knot types with given frequencies and to efficiently s... | [['a', 'lissajous', 'knot', 'is', 'one', 'that', 'can', 'be', 'parameterized', 'by', 'a', 'single', 'cosine', 'function', 'in', 'each', 'coordinate', 'lissajous', 'knots', 'are', 'highly', 'symmetric', 'and', 'for', 'this', 'reason', 'not', 'all', 'knots', 'are', 'lissajous', 'we', 'prove', 'several', 'theorems', 'whic... | [-0.24438171921659033, 0.12604399033042848, -0.09963739585435512, 0.07331363482303366, -0.10891119945718318, -0.22061812928735222, 0.07035165398419664, 0.4093128471464223, -0.2506510877592147, -0.30903593993541423, 0.07414915777947184, -0.24232524152065874, -0.14530464864397727, 0.24432578087280676, -0.0655753934402963... |
707.4211 | Expansion of the Planet Detection Channels in Next-Generation
Microlensing Surveys | We classify various types of planetary lensing signals and the channels of
detecting them. We estimate the relative frequencies of planet detections
through the individual channels with special emphasis on the new channels to be
additionally provided by future lensing experiments that will survey wide
fields continuo... | astro-ph | we classify various types of planetary lensing signals and the channels of detecting them we estimate the relative frequencies of planet detections through the individual channels with special emphasis on the new channels to be additionally provided by future lensing experiments that will survey wide fields continuousl... | [['we', 'classify', 'various', 'types', 'of', 'planetary', 'lensing', 'signals', 'and', 'the', 'channels', 'of', 'detecting', 'them', 'we', 'estimate', 'the', 'relative', 'frequencies', 'of', 'planet', 'detections', 'through', 'the', 'individual', 'channels', 'with', 'special', 'emphasis', 'on', 'the', 'new', 'channels... | [-0.16460911335347783, 0.17325207849607133, -0.05183314435931226, 0.0435843053158795, -0.10980832831647117, -0.07830828481602894, 0.09921299298848892, 0.32181809602446076, -0.2008745895108468, -0.3475520456816221, 0.11735553243183965, -0.2873543713114571, -0.10263931404509538, 0.25141839975989316, -0.03382767399578074,... |
707.4212 | Analysis of two-dimensional high-energy photoelectron momentum
distributions in single ionization of atoms by intense laser pulses | We analyzed the two-dimensional (2D) electron momentum distributions of
high-energy photoelectrons of atoms in an intense laser field using the
second-order strong field approximation (SFA2). The SFA2 accounts for the
rescattering of the returning electron with the target ion to first order and
its validity is establ... | physics.atom-ph | we analyzed the twodimensional 2d electron momentum distributions of highenergy photoelectrons of atoms in an intense laser field using the secondorder strong field approximation sfa2 the sfa2 accounts for the rescattering of the returning electron with the target ion to first order and its validity is established by c... | [['we', 'analyzed', 'the', 'twodimensional', '2d', 'electron', 'momentum', 'distributions', 'of', 'highenergy', 'photoelectrons', 'of', 'atoms', 'in', 'an', 'intense', 'laser', 'field', 'using', 'the', 'secondorder', 'strong', 'field', 'approximation', 'sfa2', 'the', 'sfa2', 'accounts', 'for', 'the', 'rescattering', 'o... | [-0.09834984295860484, 0.16484692387545602, -0.08087090410056039, 0.09348157073558033, 0.00865068869061873, -0.08752183164273139, 0.004601473379781811, 0.41353176250843937, -0.2576069374057189, -0.2520710335372993, 0.01477907796006676, -0.30736529441635635, -0.035921117684371034, 0.23115270229345056, 0.0653115229379438... |
707.4213 | A Batalin-Vilkovisky Algebra structure on the Hochschild Cohomology of
Truncated Polynomials | The main result of this paper is to calculate the Batalin-Vilkovisky
structure of $HH^*(C^*(\mathbf{K}P^n;R);C^*(\mathbf{K}P^n;R))$ for $
\mathbf{K}=\mathbb{C}$ and $\mathbb{H}$, and $R=\mathbb{Z}$ and any field; and
shows that in the special case when $M=\mathbb{C}P^1=S^2$, and $R=\mathbb{Z}$,
this structure can not... | math.AT math.GT | the main result of this paper is to calculate the batalinvilkovisky structure of hhcmathbfkpnrcmathbfkpnr for mathbfkmathbbc and mathbbh and rmathbbz and any field and shows that in the special case when mmathbbcp1s2 and rmathbbz this structure can not be identified with the bvstructure of mathbbh_ls2mathbbz computed b... | [['the', 'main', 'result', 'of', 'this', 'paper', 'is', 'to', 'calculate', 'the', 'batalinvilkovisky', 'structure', 'of', 'hhcmathbfkpnrcmathbfkpnr', 'for', 'mathbfkmathbbc', 'and', 'mathbbh', 'and', 'rmathbbz', 'and', 'any', 'field', 'and', 'shows', 'that', 'in', 'the', 'special', 'case', 'when', 'mmathbbcp1s2', 'and'... | [-0.1226808526774957, 0.07327436233892859, -0.06717826494769681, 0.0368775415672211, -0.04279580605604375, -0.056147900371191405, 0.0019108633776860578, 0.34064699625152917, -0.30560945814275847, -0.2661571809730958, 0.11842886887496293, -0.18523540056499077, -0.21279314264566415, 0.19223256843785444, -0.11703493269825... |
707.4214 | Ergodic BSDEs and Optimal Ergodic Control in Banach Spaces | In this paper we introduce a new kind of Backward Stochastic Differential
Equations, called ergodic BSDEs, which arise naturally in the study of optimal
ergodic control. We study the existence, uniqueness and regularity of solution
to ergodic BSDEs. Then we apply these results to the optimal ergodic control of
a Bana... | math.PR | in this paper we introduce a new kind of backward stochastic differential equations called ergodic bsdes which arise naturally in the study of optimal ergodic control we study the existence uniqueness and regularity of solution to ergodic bsdes then we apply these results to the optimal ergodic control of a banach valu... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'new', 'kind', 'of', 'backward', 'stochastic', 'differential', 'equations', 'called', 'ergodic', 'bsdes', 'which', 'arise', 'naturally', 'in', 'the', 'study', 'of', 'optimal', 'ergodic', 'control', 'we', 'study', 'the', 'existence', 'uniqueness', 'and', 'regularity', 'of... | [-0.20035267549101263, 0.041621990990824996, -0.07441762571688741, 0.13868547031161144, -0.13376352987252177, -0.14870665257330984, 0.07100232612719992, 0.2974506500788266, -0.42707390319556, -0.1428779473004397, 0.17733644704858306, -0.27415486637619324, -0.195732700265944, 0.18609816684038377, -0.1886427441611886, 0.... |
707.4215 | Orbit inequivalent actions of non-amenable groups | Consider two free measure preserving group actions $\Gamma \actson (X, \mu),
\Delta \actson (X, \mu)$, and a measure preserving action $\Delta \actson^a (Z,
\nu)$ where $(X, \mu), (Z, \nu)$ are standard probability spaces. We show how
to construct free measure preserving actions $\Gamma \actson^c (Y, m)$, $\Delta
\ac... | math.GR | consider two free measure preserving group actions gamma actson x mu delta actson x mu and a measure preserving action delta actsona z nu where x mu z nu are standard probability spaces we show how to construct free measure preserving actions gamma actsonc y m delta actsond y m on a standard probability space such that... | [['consider', 'two', 'free', 'measure', 'preserving', 'group', 'actions', 'gamma', 'actson', 'x', 'mu', 'delta', 'actson', 'x', 'mu', 'and', 'a', 'measure', 'preserving', 'action', 'delta', 'actsona', 'z', 'nu', 'where', 'x', 'mu', 'z', 'nu', 'are', 'standard', 'probability', 'spaces', 'we', 'show', 'how', 'to', 'const... | [-0.15243260265080208, 0.1869510034304283, -0.07518944974322248, 0.07299215286231062, -0.0606385741442647, -0.1684064021581835, 0.14335057732367187, 0.42327142441901594, -0.3151811307270524, -0.17360203559382245, 0.04111890422197383, -0.3099888050330615, -0.06244643949348172, 0.14461724882264015, -0.12261767464544658, ... |
707.4216 | Nature of the metal-nonmetal transition in metal-ammonia solutions. I.
Solvated electrons at low metal concentrations | Using a theory of polarizable fluids, we extend a variational treatment of an
excess electron to the many-electron case corresponding to finite metal
concentrations in metal-ammonia solutions (MAS). We evaluate dielectric,
optical, and thermodynamical properties of MAS at low metal concentrations. Our
semi-analytical... | cond-mat.stat-mech cond-mat.str-el | using a theory of polarizable fluids we extend a variational treatment of an excess electron to the manyelectron case corresponding to finite metal concentrations in metalammonia solutions mas we evaluate dielectric optical and thermodynamical properties of mas at low metal concentrations our semianalytical calculation... | [['using', 'a', 'theory', 'of', 'polarizable', 'fluids', 'we', 'extend', 'a', 'variational', 'treatment', 'of', 'an', 'excess', 'electron', 'to', 'the', 'manyelectron', 'case', 'corresponding', 'to', 'finite', 'metal', 'concentrations', 'in', 'metalammonia', 'solutions', 'mas', 'we', 'evaluate', 'dielectric', 'optical'... | [-0.13305426747833807, 0.16249716818517768, -0.05661825752828181, 0.04471209863750215, -0.0027342062337550694, -0.12740513429577863, 0.08503042084593622, 0.3571617586794433, -0.22793723281137843, -0.2857726451315025, -0.004793307338668792, -0.34056314412090516, -0.11435816255422733, 0.15081128353257933, 0.0264153634080... |
707.4217 | Energy-momentum of a Cosmological Brane Model and the Gauge Hierarchy | We analyze the general covariant energy-momentum tensor of the gravitational
system in genreal five-dimensional cosmological brane-world models. Then
through calculating this energy-momentum for the cosmological generalization of
the Randall-Sundrum model, which includes the original RS model as the static
limit, we ... | hep-th gr-qc | we analyze the general covariant energymomentum tensor of the gravitational system in genreal fivedimensional cosmological braneworld models then through calculating this energymomentum for the cosmological generalization of the randallsundrum model which includes the original rs model as the static limit we are able t... | [['we', 'analyze', 'the', 'general', 'covariant', 'energymomentum', 'tensor', 'of', 'the', 'gravitational', 'system', 'in', 'genreal', 'fivedimensional', 'cosmological', 'braneworld', 'models', 'then', 'through', 'calculating', 'this', 'energymomentum', 'for', 'the', 'cosmological', 'generalization', 'of', 'the', 'rand... | [-0.12916391148426376, 0.07296513013316544, -0.09037429176700804, 0.10135651602292085, -0.10090724868024444, -0.091855159075419, -0.03407837627813793, 0.2758342956428181, -0.2096062084598528, -0.2552825866860675, 0.05084377589154538, -0.2569886628067592, -0.1713179820831251, 0.13085803906637972, -0.03414618100582079, 0... |
707.4218 | N=1/2 supergravity with matter in four Euclidean dimensions | An N=1/2 supergravity in four Euclidean spacetime dimensions, coupled to both
vector- and scalar-multiplet matter, is constructed for the first time. We
begin with the standard (1,1) conformally extended supergravity in four
Euclidean dimensions, and freeze out the graviphoton field strength to an
arbitrary (fixed) s... | hep-th | an n12 supergravity in four euclidean spacetime dimensions coupled to both vector and scalarmultiplet matter is constructed for the first time we begin with the standard 11 conformally extended supergravity in four euclidean dimensions and freeze out the graviphoton field strength to an arbitrary fixed selfdual field t... | [['an', 'n12', 'supergravity', 'in', 'four', 'euclidean', 'spacetime', 'dimensions', 'coupled', 'to', 'both', 'vector', 'and', 'scalarmultiplet', 'matter', 'is', 'constructed', 'for', 'the', 'first', 'time', 'we', 'begin', 'with', 'the', 'standard', '11', 'conformally', 'extended', 'supergravity', 'in', 'four', 'euclid... | [-0.14002968942624155, 0.1936451969534434, -0.026734214598979174, 0.09563472278647288, -0.08811657372216293, -0.17377388699279323, -0.053058818290282014, 0.2987554636477989, -0.1749788613345841, -0.26772082442703254, 0.10399846798131909, -0.23509024361651526, -0.12693343626124526, 0.052553764753465126, -0.0555672408013... |
707.4219 | Real embeddings, eta invariant and Chern-Simons current | We present an alternate proof of the Bismut-Zhang localization formula for
$\eta$-invariants without using the analytic techniques developed by
Bismut-Lebeau. A Riemann-Roch property for Chern-Simons currents, which is of
independent interest, is established in due course.
| math.DG math.KT | we present an alternate proof of the bismutzhang localization formula for etainvariants without using the analytic techniques developed by bismutlebeau a riemannroch property for chernsimons currents which is of independent interest is established in due course | [['we', 'present', 'an', 'alternate', 'proof', 'of', 'the', 'bismutzhang', 'localization', 'formula', 'for', 'etainvariants', 'without', 'using', 'the', 'analytic', 'techniques', 'developed', 'by', 'bismutlebeau', 'a', 'riemannroch', 'property', 'for', 'chernsimons', 'currents', 'which', 'is', 'of', 'independent', 'int... | [-0.13872822314604288, 0.07467573603409822, -0.12254644330177042, 0.07961389699873204, -0.07424126578391427, -0.12374586113987283, 0.02972263532380263, 0.2917126942839887, -0.18665680387574765, -0.23796284586812058, 0.11061795106636257, -0.15697643991249302, -0.1852415251131687, 0.2534478074974484, -0.12832572143007484... |
707.422 | The BOES spectropolarimeter for Zeeman measurements of stellar magnetic
fields | We introduce a new polarimeter installed on the high-resolution fiber-fed
echelle spectrograph (called BOES) of the 1.8-m telescope at the Bohyunsan
Optical Astronomy Observatory, Korea. The instrument is intended to measure
stellar magnetic fields with high-resolution (R $\sim$ 60000)
spectropolarimetric observation... | astro-ph | we introduce a new polarimeter installed on the highresolution fiberfed echelle spectrograph called boes of the 18m telescope at the bohyunsan optical astronomy observatory korea the instrument is intended to measure stellar magnetic fields with highresolution r sim 60000 spectropolarimetric observations of intrinsic p... | [['we', 'introduce', 'a', 'new', 'polarimeter', 'installed', 'on', 'the', 'highresolution', 'fiberfed', 'echelle', 'spectrograph', 'called', 'boes', 'of', 'the', '18m', 'telescope', 'at', 'the', 'bohyunsan', 'optical', 'astronomy', 'observatory', 'korea', 'the', 'instrument', 'is', 'intended', 'to', 'measure', 'stellar... | [-0.13040326955692413, 0.1443445713733896, -0.051015876506705984, 0.026742371417080555, -0.145263205962972, -0.10496385177472033, -0.012951670151848633, 0.4362903604543625, -0.16111305438411924, -0.4122248344983046, 0.09996764998672567, -0.306666446921344, -0.0411989587591961, 0.26816475415566504, -0.04316341071926917,... |
707.4221 | A comment on the matter-graviton coupling | We point out a generic inconsistency of the coupling of ordinary gravity as
described by general relativity with matter invariant under the subgroup of
unimodular diffeomorphisms (TDiffs), and some previously studied exceptions are
pointed out. The most general Lagrangian invariant under TDiff up to dimension
five op... | hep-th | we point out a generic inconsistency of the coupling of ordinary gravity as described by general relativity with matter invariant under the subgroup of unimodular diffeomorphisms tdiffs and some previously studied exceptions are pointed out the most general lagrangian invariant under tdiff up to dimension five operator... | [['we', 'point', 'out', 'a', 'generic', 'inconsistency', 'of', 'the', 'coupling', 'of', 'ordinary', 'gravity', 'as', 'described', 'by', 'general', 'relativity', 'with', 'matter', 'invariant', 'under', 'the', 'subgroup', 'of', 'unimodular', 'diffeomorphisms', 'tdiffs', 'and', 'some', 'previously', 'studied', 'exceptions... | [-0.168390008246862, 0.11902508901462691, -0.05604603410255714, 0.10101669850629434, -0.08099167124887348, -0.18307268099676147, -0.00644789275820138, 0.31377099229206074, -0.23186805926942738, -0.28046402194705167, 0.12903351071634192, -0.2825303172967473, -0.127408170862673, 0.19515639554220635, -0.07357142748097416,... |
707.4222 | Long-range order in the A-like phase of superfluid 3He in aerogel | A mutual action of the random anisotropy brought in the superfluid 3He by
aerogel and of the global anisotropy caused by its deformation is considered.
Strong global anisotropy tends to suppress fluctuations of orientation of the
order parameter and stabilizes ABM order parameter. In a limit of vanishing
anisotropy t... | cond-mat.dis-nn | a mutual action of the random anisotropy brought in the superfluid 3he by aerogel and of the global anisotropy caused by its deformation is considered strong global anisotropy tends to suppress fluctuations of orientation of the order parameter and stabilizes abm order parameter in a limit of vanishing anisotropy these... | [['a', 'mutual', 'action', 'of', 'the', 'random', 'anisotropy', 'brought', 'in', 'the', 'superfluid', '3he', 'by', 'aerogel', 'and', 'of', 'the', 'global', 'anisotropy', 'caused', 'by', 'its', 'deformation', 'is', 'considered', 'strong', 'global', 'anisotropy', 'tends', 'to', 'suppress', 'fluctuations', 'of', 'orientat... | [-0.23312513524901934, 0.24060346686613115, -0.08716121009797201, 0.051962385405037, -0.043350458177256176, -0.06223936749879142, 0.014789900180466217, 0.2837510423349409, -0.28533295712208956, -0.2880919035738227, 0.07412348214226465, -0.2943338257014409, -0.07425830901825223, 0.0783381801334092, 0.009589614332907823,... |
707.4223 | Spatial reflection and renormalization group flow of quantum many-body
systems with matrix product state representation | The property of quantum many-body systems under spatial reflection and the
relevant physics of renormalization group (RG) procedure are revealed. By
virtue of the matrix product state (MPS) representation, various attributes for
translational invariant systems associated with spatial reflection are
manifested. We dem... | quant-ph cond-mat.stat-mech | the property of quantum manybody systems under spatial reflection and the relevant physics of renormalization group rg procedure are revealed by virtue of the matrix product state mps representation various attributes for translational invariant systems associated with spatial reflection are manifested we demonstrate s... | [['the', 'property', 'of', 'quantum', 'manybody', 'systems', 'under', 'spatial', 'reflection', 'and', 'the', 'relevant', 'physics', 'of', 'renormalization', 'group', 'rg', 'procedure', 'are', 'revealed', 'by', 'virtue', 'of', 'the', 'matrix', 'product', 'state', 'mps', 'representation', 'various', 'attributes', 'for', ... | [-0.17902750500406212, 0.1476263199206237, -0.15330035818720256, 0.03896811269837749, -0.02054262364150158, -0.1328393673769884, 0.06515490571497479, 0.39138491378053203, -0.3091359304591686, -0.25217790293550774, 0.08941936546522142, -0.2494936530161035, -0.16861088517132206, 0.1290717607998586, 0.0010836895611706435,... |
707.4224 | The $\phi$ - Meson Physics in the Chirial Model | The $\phi \to K^+K^-,K^{0}_{L},K^{0}_{S},K^{0}\bar K^0$ decays are studied
using the method of phenomenological chiral Lagrangians. Calculated values for
partial widths for these decay channels are compared with available
experimental data.
| hep-ph | the phi to kkk0_lk0_sk0bar k0 decays are studied using the method of phenomenological chiral lagrangians calculated values for partial widths for these decay channels are compared with available experimental data | [['the', 'phi', 'to', 'kkk0_lk0_sk0bar', 'k0', 'decays', 'are', 'studied', 'using', 'the', 'method', 'of', 'phenomenological', 'chiral', 'lagrangians', 'calculated', 'values', 'for', 'partial', 'widths', 'for', 'these', 'decay', 'channels', 'are', 'compared', 'with', 'available', 'experimental', 'data']] | [-0.09582979146969216, 0.17287199674495335, -0.02281616184988926, 0.09457204561552097, -0.04163521798006419, -0.20417803098800882, -0.02751038272881174, 0.4071276501174374, -0.1980945267553987, -0.238962150082506, 0.024336009101685267, -0.389465959164603, 0.03393219832074026, 0.21310959990810732, 0.13936307718013896, 0... |
707.4225 | Electron-Electron Bremsstrahlung Emission and the Inference of Electron
Flux Spectra in Solar Flares | Although both electron-ion and electron-electron bremsstrahlung contribute to
the hard X-ray emission from solar flares, the latter is normally ignored. Such
an omission is not justified at electron (and photon) energies above $\sim 300$
keV, and inclusion of the additional electron-electron bremsstrahlung in
general... | astro-ph | although both electronion and electronelectron bremsstrahlung contribute to the hard xray emission from solar flares the latter is normally ignored such an omission is not justified at electron and photon energies above sim 300 kev and inclusion of the additional electronelectron bremsstrahlung in general makes the ele... | [['although', 'both', 'electronion', 'and', 'electronelectron', 'bremsstrahlung', 'contribute', 'to', 'the', 'hard', 'xray', 'emission', 'from', 'solar', 'flares', 'the', 'latter', 'is', 'normally', 'ignored', 'such', 'an', 'omission', 'is', 'not', 'justified', 'at', 'electron', 'and', 'photon', 'energies', 'above', 's... | [-0.050161808868665, 0.21397685162973845, -0.03490455523605093, 0.18807548308211158, -0.03226458618998433, -0.11456259134705568, 0.03979649418751639, 0.42111679349024883, -0.21855439335961174, -0.3746453643928278, -0.023306964418649805, -0.3321280519289297, 0.040863955519592904, 0.22791390205909895, 0.044517468938005, ... |
707.4226 | A Unified Algebraic Approach to Classical Yang-Baxter Equation | In this paper, the different operator forms of classical Yang-Baxter equation
are given in the tensor expression through a unified algebraic method. It is
closely related to left-symmetric algebras which play an important role in many
fields in mathematics and mathematical physics. By studying the relations
between l... | math.QA math-ph math.MP | in this paper the different operator forms of classical yangbaxter equation are given in the tensor expression through a unified algebraic method it is closely related to leftsymmetric algebras which play an important role in many fields in mathematics and mathematical physics by studying the relations between leftsymm... | [['in', 'this', 'paper', 'the', 'different', 'operator', 'forms', 'of', 'classical', 'yangbaxter', 'equation', 'are', 'given', 'in', 'the', 'tensor', 'expression', 'through', 'a', 'unified', 'algebraic', 'method', 'it', 'is', 'closely', 'related', 'to', 'leftsymmetric', 'algebras', 'which', 'play', 'an', 'important', '... | [-0.14046310237719722, 0.0247474615265327, -0.12873465194508235, 0.13346390323824295, -0.17686058534752755, -0.15868596220389009, -0.07384756135510369, 0.2970017424740252, -0.3947273308499938, -0.22516454011201859, 0.07930672798372274, -0.2066421204534847, -0.2606145230432351, 0.22245486565821226, -0.12743845123442865,... |
707.4227 | Magnetization and Magnetoscrition of van Vleck antiferromagnets with
magnetic anisotropy of "easy-plane" type | The theoretical description of quantum phase transition, induced by the
external magnetic field, into antiferromagnetic state in the van Vleck -
singlet - magnet with a single-ion anisotropy of "easy-plane" type and ion spin
S=1 is proposed. It is shown that the spin polarization of the ground
non-degenerated state p... | cond-mat.stat-mech | the theoretical description of quantum phase transition induced by the external magnetic field into antiferromagnetic state in the van vleck singlet magnet with a singleion anisotropy of easyplane type and ion spin s1 is proposed it is shown that the spin polarization of the ground nondegenerated state proves to be the... | [['the', 'theoretical', 'description', 'of', 'quantum', 'phase', 'transition', 'induced', 'by', 'the', 'external', 'magnetic', 'field', 'into', 'antiferromagnetic', 'state', 'in', 'the', 'van', 'vleck', 'singlet', 'magnet', 'with', 'a', 'singleion', 'anisotropy', 'of', 'easyplane', 'type', 'and', 'ion', 'spin', 's1', '... | [-0.18428702381658438, 0.20044262450869949, -0.05620575713257847, 0.024264223994374442, -0.0579843663857249, -0.1006530961021781, 0.013213566811963805, 0.371810648576426, -0.23690316130740763, -0.2814999582704657, 0.042349523576254496, -0.30387339891115234, -0.10398732182750506, 0.17732710793002773, 0.09518227683825058... |
707.4228 | Comparison of RABITT and FROG measurements in the temporal
characterization of attosecond pulse trains | The attosecond high harmonic pulses obtained from a long Ar-filled gas cell
were characterized by two techniques - the reconstruction of attosecond beating
by interference of two-photon transition (RABITT) and frequency-resolved
optical gating (FROG) methods. The pulse durations obtained by RABITT and FROG
methods ag... | physics.optics physics.atom-ph | the attosecond high harmonic pulses obtained from a long arfilled gas cell were characterized by two techniques the reconstruction of attosecond beating by interference of twophoton transition rabitt and frequencyresolved optical gating frog methods the pulse durations obtained by rabitt and frog methods agreed within ... | [['the', 'attosecond', 'high', 'harmonic', 'pulses', 'obtained', 'from', 'a', 'long', 'arfilled', 'gas', 'cell', 'were', 'characterized', 'by', 'two', 'techniques', 'the', 'reconstruction', 'of', 'attosecond', 'beating', 'by', 'interference', 'of', 'twophoton', 'transition', 'rabitt', 'and', 'frequencyresolved', 'optic... | [-0.04954821467528948, 0.23345514751142926, -0.052117564239435726, 0.08519198473335968, 0.09484227119634549, -0.22201587598149974, 0.08430533659023544, 0.5530924207634396, -0.23899774191280207, -0.301512555198537, 0.033150177645600507, -0.23932863971114987, -0.13193178218271998, 0.27358240162332853, -0.0465597176044765... |
707.4229 | Giant Magneto-impedance in stress-annealed Finemet/Copper/Finemet based
trilayer structures | The resistive and reactive components of magneto-impedance (MI) for
Finemet/Copper/Finemet sandwiched structures based on stress-annealed
nanocrystalline Fe75Si15B6Cu1Nb3 ribbons as functions of different fields
(longitudinal and perpendicular) and frequencies have been measured and
analyzed. Maximum magneto-resistan... | cond-mat.mtrl-sci | the resistive and reactive components of magnetoimpedance mi for finemetcopperfinemet sandwiched structures based on stressannealed nanocrystalline fe75si15b6cu1nb3 ribbons as functions of different fields longitudinal and perpendicular and frequencies have been measured and analyzed maximum magnetoresistance and magne... | [['the', 'resistive', 'and', 'reactive', 'components', 'of', 'magnetoimpedance', 'mi', 'for', 'finemetcopperfinemet', 'sandwiched', 'structures', 'based', 'on', 'stressannealed', 'nanocrystalline', 'fe75si15b6cu1nb3', 'ribbons', 'as', 'functions', 'of', 'different', 'fields', 'longitudinal', 'and', 'perpendicular', 'an... | [-0.1536146413407051, 0.1774315137805697, 0.046967051682835506, 0.011159991388957874, -0.06928105242215583, -0.07155571336511012, 0.03039646309532615, 0.39743969477773977, -0.2312917447697639, -0.3639456226058256, 0.08011964314124163, -0.24822264654695794, -0.05859148530959109, 0.23735174177567553, 0.032815648574576854... |
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