Search results for "INELASTIC"

showing 10 items of 700 documents

Inelastic neutron scattering measurements on Nd2Fe14B and Y2Fe14B single crystals

1992

Abstract Inelastic neutron scattering measurements have been carried out on Nd 2 Fe 14 B and Y 2 Fe 14 B single crystals. Temperature dependent acoustic magnon dispersion curves have been found along the high-symmetry directions [0,0,1] and [1,0,0] with a gap at (0,0,2). Soft mode behaviour at spin wave vector q = 0 was observed for Nd 2 Fe 14 B near the spin reorientation temperature. The inelastic scattering intensity decreases steeply for larger q . Therefore, the dispersion curves could be measured until the middle of the Brillouin zone only. The experimental results are discussed in the frame of a classical spin wave model.

Resonant inelastic X-ray scatteringPhysicsQuasielastic scatteringCondensed matter physicsMagnonDynamic structure factorQuasielastic neutron scatteringInelastic scatteringCondensed Matter PhysicsSmall-angle neutron scatteringInelastic neutron scatteringElectronic Optical and Magnetic MaterialsJournal of Magnetism and Magnetic Materials
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"Table 1" of "A Measurement of the tau leptonic branching fractions"

1995

Axis error includes +- 0.23/0.23 contribution (Data statistics).

SIG/SIGElectron productionIntegrated Cross SectionDeep Inelastic ScatteringCross Section91.0InclusiveE+ E- --> TAU- TAU+E+ E- ScatteringNeutral CurrentE+ E- --> ZExclusiveTau productionE+ E- --> E- NUTAU NUEBAR XE+ E- --> E+ NUTAUBAR NUE X
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Electron resonance scattering from mercury

1977

The differential cross section and the spin polarisation of electrons scattered elastically from mercury have been measured as a function of collision energy in the range 4.0 to 6.0 eV for several selected scattering angles. The observed data can be understood if one assumes that resonances are formed at 4.55 eV in the 2S1/2, at 4.71 eV in the 2D3/2 and at 4.94 eV and 5.51 eV respectively in the 2D5/2 scattering state.

Scattering cross-sectionElastic scatteringPhysicsElectron resonancechemistryScatteringchemistry.chemical_elementResonance scatteringElectronInelastic scatteringAtomic physicsAtomic and Molecular Physics and OpticsMercury (element)Journal of Physics B: Atomic and Molecular Physics
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Transport of Mobile Particles in an Immobile Environment: Computer Simulations of Sodium Silicates

2007

Molecular dynamics (MD) simulations of various sodium silicate melts, (Na2O)x(SiO2) with x=2, 3, 20, are presented. In these systems, the mobility of sodium ions is much higher, often by orders of magnitude, than that of the silicon and oxygen atoms forming a tetrahedral network structure. We show that the high mobility of sodium is intimately related to the chemical ordering in sodium silicates. A network of percolating sodium-rich channels is formed in the static structure that serve as diffusion channels for the sodium ions. This channel network is revealed in static structure factors by a prepeak at the wavenumber q=0.95 A-1. Inelastic neutron scattering experiments of sodium silicate m…

ScatteringSodiumIncoherent scatterchemistry.chemical_elementmolecular dynamics computer simulationSodium silicatedynamicsmode coupling theoryInelastic neutron scatteringIonchemistry.chemical_compoundCrystallographysilicate meltschemistryChemical physicsPhysics::Atomic and Molecular ClustersDiffusion (business)Structure factor
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Relativistic multipole operators for semileptonic weak and electromagnetic nuclear reactions.

1989

We discuss multipole operators that arise in a relativistic analysis ofsemileptonic weak and electromagnetic interactions with nuclei. Thesesingle-particle operators are evaluated between relativistic nucleon boundstates that are solutions to the Dirac equation with potentials of the formproduced by the sigma-..omega.. model. The reduced matrix elements aregiven in terms of easily programmable radial integrals and can be applied to anumber of reactions such as elastic and inelastic electron scattering, realphoton processes, ..beta.. decay, and charged lepton capture as well as moreexotic interactions such as charged and neutral current neutrino reactions. Asa specific example, we calculate …

Semileptonic decayPhysicsElastic scatteringNuclear and High Energy PhysicsParticle physicsNeutral currentNuclear TheoryInelastic scatteringsymbols.namesakeQuantum electrodynamicsDirac equationsymbolsNeutrinoMultipole expansionLeptonPhysical review. C, Nuclear physics
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Spin–isospin excitations probed by strong, weak and electro-magnetic interactions

2011

Abstract Gamow–Teller (GT) transitions are the most common weak interaction processes of spin–isospin ( σ τ ) type in atomic nuclei. They are of interest not only in nuclear physics but also in astrophysics; they play an important role in supernovae explosions and nucleosynthesis. The direct study of weak decay processes, however, gives relatively limited information about GT transitions and the states excited via GT transitions (GT states); β decay can only access states at excitation energies lower than the decay Q -value, and neutrino-induced reactions have very small cross-sections. However, one should note that β decay has a direct access to the absolute GT transition strengths B (GT) …

Semileptonic decayPhysicsNuclear and High Energy PhysicsExcited stateIsospinAtomic nucleusIsobarWeak interactionAtomic physicsInelastic scatteringQuantum numberProgress in Particle and Nuclear Physics
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Ferroelastic transition in Kbr:Kcn studied by neutrons, x-rays and ultrasonic

1986

The ferroelastic phase transition of (KBr) 0 27 (KNC) 0.73 has been studied by X-ray diffraction, ultrasonics and inelastic neutron scattering. It is the first example of a cubic crystal where the elastic shear constant C 44 softens completely corresponding to the m = 2 universality class. C 44 and the Bragg intensities show a non-classical critical behaviour.

Shear (sheet metal)DiffractionPhase transitionMaterials scienceCondensed matter physicsAstrophysics::High Energy Astrophysical PhenomenaGeneral EngineeringNeutronCubic crystal systemRenormalization groupConstant (mathematics)Inelastic neutron scattering
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Capturing blast waves in granular flow

2007

Abstract In this paper we continue the analysis of compressible Euler equations for inelastic granular gases described by a granular equation of state due to Goldshtein and Shapiro [Goldshtein A, Shapiro M. Mechanics of collisional motion of granular materials. Part 1: General hydrodynamic equations. J Fluid Mech 1995;282:75–114], and an energy loss term accounting for inelastic collisions. We study the hydrodynamics of blast waves in granular gases by means of a fifth-order accurate scheme that resolves the evolution under different restitution coefficients. We have observed and analyzed the formation of a cluster region near the contact wave using the one-dimensional and two-dimensional v…

Shock wavePhysicsEquation of stateGeneral Computer ScienceGeneral EngineeringInelastic collisionMechanicsGranular materialEuler equationssymbols.namesakeClassical mechanicsCompressibilitysymbolsFluidizationBlast waveComputers & Fluids
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Capturing shock waves in inelastic granular gases

2005

Shock waves in granular gases generated by hitting an obstacle at rest are treated by means of a shock capturing scheme that approximates the Euler equations of granular gas dynamics with an equation of state (EOS), introduced by Goldshtein and Shapiro [J. Fluid Mech. 282 (1995) 75-114], that takes into account the inelastic collisions of granules. We include a sink term in the energy balance to account for dissipation of the granular motion by collisional inelasticity, proposed by Haff [J. Fluid Mech. 134 (1983) 401-430], and the gravity field added as source terms. We have computed the approximate solution to a one-dimensional granular gas falling on a plate under the acceleration of grav…

Shock wavePhysicsNumerical AnalysisEquation of statePhysics and Astronomy (miscellaneous)Applied MathematicsInelastic collisionEnergy balanceGas dynamicsDissipationComputer Science ApplicationsEuler equationsComputational Mathematicssymbols.namesakeClassical mechanicsGravitational fieldModeling and SimulationsymbolsJournal of Computational Physics
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"Table 36" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Compilation of multiplicities of pseudoscalar mesons from current LEP I data.

Strange productionElectron productionHigh Energy Physics::LatticeNuclear Theory91.2MULTInclusiveE+ E- --> B+ XE+ E- --> D+ XE+ E- --> B0 XE+ E- --> B- XE+ E- --> D0 XE+ E- --> K0 XE+ E- --> K- XHigh Energy Physics::PhenomenologyE+ E- --> ETAPRIME XE+ E- --> K+ XDeep Inelastic ScatteringE+ E- --> ETA XE+ E- --> PI- XE+ E- --> PI+ XE+ E- --> PI0 XCharm productionE+ E- ScatteringComputer Science::Programming LanguagesHigh Energy Physics::Experiment
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