Search results for "waves"

showing 10 items of 1766 documents

The boson peak

2013

The vibrational properties of glasses in the THz range differ very much from what is expected from Debye's elasticity theory: the density of states (DOS) deviates from Debye's ω2 law [the “boson peak” (BP)], the sound velocity shows a negative dispersion in the BP frequency regime and there is a strong increase in the sound attenuation near the BP frequency. These anomalies are related to an anomalous temperature dependence of the specific heat and thermal conductivity in the 10 K regime. An overview of the heterogeneous-elasticity theory is given, by means of which all these anomalies can be explained and shown to arise from the structural disorder, leading to spatial fluctuations of the s…

PhysicsRange (particle radiation)Condensed matter physicsCondensed Matter PhysicsSymmetry (physics)Electronic Optical and Magnetic MaterialsShear modulussymbols.namesakeThermal conductivityQuantum electrodynamicsDensity of statessymbolsDispersion (water waves)Acoustic attenuationDebyephysica status solidi (b)
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Isotopic distributions of thermal-neutron-induced fission fragments of near-symmetric fission of Pu239,241 determined using calorimetric low-temperat…

2021

Isotopic distributions were measured for the light fragment group in the transition region from asymmetric to symmetric fission for thermal neutron induced fission of $^{239}\mathrm{Pu}$ and $^{241}\mathrm{Pu}$ using the novel technology of calorimetric low temperature detectors in combination with the passive absorber method. Nuclear charge distributions were determined for 24 masses in the range $A=89$ to $A=112$ for $^{241}\mathrm{Pu}({n}_{\mathrm{th}},f)$ for the first time with the LOHENGRIN mass spectrometer. Moving from asymmetric to symmetric fission, known data were supplemented for masses from $A=110$ to $A=112$ for $^{241}\mathrm{Pu}({n}_{\mathrm{th}},f)$ and from $A=109$ to $A=1…

PhysicsRange (particle radiation)IsotopeProton010308 nuclear & particles physicsFissionCharge (physics)Polarization (waves)7. Clean energy01 natural sciencesNeutron temperatureEffective nuclear charge0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsPhysical Review C
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Conversion of bright magneto-optical resonances into dark resonances at fixed laser frequency forD2excitation of atomic rubidium

2012

Nonlinear magneto-optical resonances on the hyperfine transitions belonging to the ${D}_{2}$ line of rubidium were changed from bright to dark resonances by changing the laser power density of the single exciting laser field or by changing the vapor temperature in the cell. In one set of experiments atoms were excited by linearly polarized light from an extended cavity diode laser with polarization vector perpendicular to the light's propagation direction and magnetic field, and laser-induced fluorescence was observed along the direction of the magnetic field, which was scanned. A low-contrast bright resonance was observed at low laser power densities when the laser was tuned to the ${F}_{g…

PhysicsResonanceLaserPolarization (waves)Atomic and Molecular Physics and OpticsMagnetic fieldlaw.inventionlawExcited statePhysics::Atomic PhysicsAtomic physicsHyperfine structureExcitationCircular polarizationPhysical Review A
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Numerical study of the stability of the Peregrine solution

2017

International audience; The Peregrine solution to the nonlinear Schrödinger equations is widely discussed as a model for rogue waves in deep water. We present here a detailed fully nonlinear numerical study of high accuracy of perturbations of the Peregrine solution as a solution to the nonlinear Schrödinger (NLS) equations.We study localized and nonlocalized perturbations of the Peregrine solution in the linear and fully nonlinear setting. It is shown that the solution is unstable against all considered perturbations.

PhysicsRogue wavesGeneral Medicine01 natural sciencesStability (probability)010305 fluids & plasmasDeep waterSchrödinger equationsymbols.namesakeNonlinear systemClassical mechanics[ MATH.MATH-AP ] Mathematics [math]/Analysis of PDEs [math.AP]Peregrine solution0103 physical sciencessymbolsNonlinear Schrödinger equation[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Rogue wave010306 general physicsNonlinear Sciences::Pattern Formation and SolitonsNonlinear Schrödinger equationSchrödinger's cat
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Collisions and Mechanical Wave Propagation in Elastic Rods

2011

Some results from experiments intended to measure the propagation speed of sound waves produced by collisions between small bodies and metallic rods are analysed. Elementary models of elastic collision and of the reflection and transmission of waves at media boundaries are discussed and tested with experimental data, in the framework of a workshop on mechanical wave propagation that featured at the University of Palermo in a two-year graduate programme for prospective physics teachers and in courses for undergraduate engineering and physics students.

PhysicsSPEED OF SOUND IN METALSSettore FIS/08 - Didattica E Storia Della FisicaMechanical EngineeringAcousticsPhysics educationMeasure (physics)CONSTRAINTSPHYSICS EDUCATIONPhysics::Physics EducationRodEducationElastic collisionSpeed of soundReflection (physics)Elastic rodsMechanical waveMECHANICAL WAVESInternational Journal of Mechanical Engineering Education
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Low Energy Behaviour of the Phase Shifts for Velocity-Dependent Potentials

1973

PhysicsScattering amplitudeElastic scatteringLow energyPhysics and Astronomy (miscellaneous)Phonon scatteringPhase (waves)Scattering lengthInelastic scatteringAtomic physicsProgress of Theoretical Physics
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Scattering of unstable particles in a finite volume: The case ofπρscattering and thea1(1260)resonance

2012

We present a way to evaluate the scattering of unstable particles quantized in a finite volume with the aim of extracting physical observables for infinite volume from lattice data. We illustrate the method with the $\ensuremath{\pi}\ensuremath{\rho}$ scattering which generates dynamically the axial-vector ${a}_{1}(1260)$ resonance. Energy levels in a finite box are evaluated both considering the $\ensuremath{\rho}$ as a stable and unstable resonance and we find significant differences between both cases. We discuss how to solve the problem to get the physical scattering amplitudes in the infinite volume, and hence phase shifts, from possible lattice results on energy levels quantized insid…

PhysicsScattering amplitudeNuclear and High Energy PhysicsFinite volume methodBethe–Salpeter equationScatteringLattice gauge theoryQuantum mechanicsLattice (order)Phase (waves)ObservablePhysical Review D
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Role of pion exchange inηmeson photoproduction on the deuteron

2015

Incoherent $\ensuremath{\eta}$ photoproduction on the deuteron is studied, with the main emphasis on the role of final-state interactions. In addition to the previously studied mechanisms of $NN$ and $\ensuremath{\eta}N$ rescatterings, the role of an intermediate pion exchange is considered in detail, where first a pion is photoproduced on one nucleon and then rescatters into an $\ensuremath{\eta}$ meson on the other, the spectator nucleon. It is found that the role of this pion-mediated contribution is comparable in size to that of $\ensuremath{\eta}N$ rescattering. Results for total and semi-inclusive differential cross sections and associated polarization observables are presented. In pa…

PhysicsScattering cross-sectionNuclear and High Energy PhysicsParticle physicsMeson productionMesonNuclear TheoryPolarization observablesPolarization (waves)Nuclear physicsPionDeuteriumHigh Energy Physics::ExperimentNuclear ExperimentNucleonPhysical Review C
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Photoproduction of η and η′ mesons with EtaMAID

2016

The unitary isobar model EtaMAID has been updated with an extended list of nucleon resonances, fitted to recent and new data for differential cross sections and polarization observables. The nonresonant background is described by Regge trajectories of ω,ρ and a 1 , b 1 mesons and in addition Regge cuts, where vector and axial vector mesons are exchanged together with Pomeron and f 2 mesons.

PhysicsScattering cross-sectionParticle physicsMeson010308 nuclear & particles physicsHigh Energy Physics::LatticePhysicsQC1-999Polarization observablesNuclear TheoryHigh Energy Physics::PhenomenologyPolarization (waves)01 natural sciencesNuclear physicsPomeron0103 physical sciencesIsobarHigh Energy Physics::Experiment010306 general physicsNucleonNuclear ExperimentPseudovectorEPJ Web of Conferences
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Effects of Higher-Order Scattering in a Molecular Atmosphere

1964

The effects of higher-order scattering on intensity, degree of polarization, and direction of the plane of polarization in a molecular atmosphere have been calculated.Inclusion of higher-order scattering changes these parameters strongly. Particularly, consideration of higher-order scattering is essential in the blue wavelength range (large optical thickness). The influence increases with decreasing zenith distance of the sun. The earth albedo augments the effect, except for direction of the polarization, which is independent of higher-order scattering.

PhysicsScatteringbusiness.industryGeneral EngineeringPolarization (waves)Electromagnetic radiationMolecular physicsLight scatteringOpticsDegree of polarizationAstrophysics::Earth and Planetary AstrophysicsRayleigh sky modelbusinessOptical depthZenithJournal of the Optical Society of America
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