Search results for "Elastic collision"

showing 10 items of 18 documents

Which physical parameters can be inferred from the emission variability of relativistic jets?

2005

We present results of a detailed numerical study and theoretical analysis of the dynamics of internal shocks in relativistic jets and the non-thermal flares associated with these shocks. In our model internal shocks result from collisions of density inhomogeneities (shells) in relativistic jet flows. We find that the merged shell resulting from the inelastic collision of shells has a complicated internal structure due to the non-linear dynamics of the interaction. Furthermore, the instantaneous efficiency for converting kinetic energy into thermal energy is found to be almost twice as high as theoretically expected during the period of significant emission. The Lorentz factors of the intern…

PhysicsJet (fluid)Inertial frame of referencebusiness.industryLorentz transformationAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)Inelastic collisionShell (structure)FOS: Physical sciencesAstronomy and AstrophysicsAstrophysicsKinetic energyAstrophysicsComputational physicssymbols.namesakeAstrophysical jetSpace and Planetary SciencesymbolsbusinessThermal energy
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Rotational Transitions of CO+Induced by Atomic Hydrogen

2008

The CO+ molecular ion has been observed in photon-dominated regions. Recent modeling has not been able to explain the abundances of CO+ in these regions. The most abundant collision partners are believed to be hydrogen atoms, hydrogen molecules, and electrons. The reactions of these species with CO+ have been studied previously and found to be fast. The only inelastic processes studied before were collisions of CO+ with electrons. Here we investigate the inelastic collisions of CO+ with hydrogen atoms. We argue that this can be done on the lowest triplet electronic state. This implies that CO+ ions, in a hydrogen atom dominated surrounding, experiences a few inelastic collisions before reac…

PhysicsHydrogenPolyatomic ionInelastic collisionRotational transitionchemistry.chemical_elementAstronomy and AstrophysicsRotational temperatureHydrogen atomIonchemistrySpace and Planetary SciencePotential energy surfaceAtomic physicsThe Astrophysical Journal
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Multi-Scale Modeling of Quantum Semiconductor Devices

2006

This review is concerned with three classes of quantum semiconductor equations: Schrodinger models, Wigner models, and fluid-type models. For each of these classes, some phenomena on various time and length scales are presented and the connections between micro-scale and macro-scale models are explained. We discuss Schrodinger-Poisson systems for the simulation of quantum waveguides and illustrate the importance of using open boundary conditions. We present Wigner-based semiconductor models and sketch their mathematical analysis. In particular we discuss the Wigner-Poisson-Focker-Planck system, which is the starting point of deriving subsequently the viscous quantum hydrodynamic model. Furt…

PhysicsOpen quantum systemsymbols.namesakeSemiconductor device modelingInelastic collisionsymbolsWigner distribution functionBoundary value problemStatistical physicsSemiconductor process simulationQuantumSchrödinger's cat
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Positrons and Electrons Emitted in Elastic and Dissipative Heavy Ion Collisions

1987

The main research line of the Tori group is the study of the reaction dynamics of dissipative collisions between heavy ions ia positron and electron spectroscopy. The last five years since the Lahnstein-Conference1 are marked for our group by the installation of a new experimental device for detecting positrons and electrons emitted in these collisions, the so-called Tori spectrometer2. The first part of this report is devoted therefore to describe the main characteristics of this apparatus.

PhysicsElastic scatteringPositronDissipative systemElectronImpact parameterAtomic physicsNuclear ExperimentElectron spectroscopyElastic collisionIon
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Collisional Broadening of Rotational Lines in the Stimulated Raman Pentad Q-Branch of CD4

1992

Self- and argon-broadening coefficients are reported for a number of Raman Q-branch transitions in the nu(1) and nu(2) + nu(4) bands of (C-12)D4 at room temperature (296 K). The coefficients display a variation with j and with C exp n (symmetry species A, E, F) that is essentially independent of collision partner and which is similar to the j- and C exp n-dependence found in previous measurements of the IR line-broadening coefficients. The rotationally inelastic collision rates previously measured by Foy et al. (1988) for (C-13)D4 (V4 = 0, 1) in collision with (C-13)D4 or Ar account for only a part of the Raman broadening rate, suggesting possibly significant contributions to the linewidths…

DephasingInelastic collision02 engineering and technologyLORENTZ WIDTH01 natural sciencesLOW-TEMPERATURESSpectral linesymbols.namesakeNuclear magnetic resonance0103 physical sciencesSPECTRAStimulated ramanPhysicsTUNABLE-DIODE-LASERRadiationSPECTROSCOPY010304 chemical physicsINFRARED DOUBLE-RESONANCESpectral bands021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsSymmetry (physics)METHANE LINESCM-1 REGIONsymbolsSHIFT COEFFICIENTSAtomic physics0210 nano-technologyRaman spectroscopyENERGY-TRANSFER
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The Phenomenology of Elastic Energy Loss

2007

The unexpectedly strong suppression of high p_T heavy-quarks in heavy-ion collisions has given rise to the idea that partons propagating through a medium in addition to energy loss by induced radiation also undergo substantial energy loss due to elastic collisions. However, the precise magnitude of this elastic energy loss component is highly controversial. While it is for a parton inside a medium surprisingly difficult to define the difference between elastic and radiative processes rigorously, the main phenomenological difference is in the dependence of energy loss on in-medium pathlength: in a constant medium radiative energy loss is expected to grow quadratically with pathlength, elasti…

PhysicsQuarkNuclear and High Energy PhysicsHadronElastic energyRadiant energyFOS: Physical sciencesPartonElastic collisionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Path lengthQuantum electrodynamicsRadiative transferNuclear Experiment
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Exact results for the homogeneous cooling state of an inelastic hard-sphere gas

1998

The infinite set of moments of the two-particle distribution function is found exactly for the uniform cooling state of a hard-sphere gas with inelastic collisions. Their form shows that velocity correlations cannot be neglected, and consequently the 'molecular chaos' hypothesis leading to the inelastic Boltzmann and Enskog kinetic equations must be questioned. © 1998 Cambridge University Press.

Physicssymbols.namesakeInfinite setClassical mechanicsDistribution functionBoltzmann constantsymbolsInelastic collisionMolecular chaosHard spheresInelastic scatteringCondensed Matter PhysicsBoltzmann equationJournal of Plasma Physics
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Scaling laws for inelastic collision processes in diatomic molecules

1991

International audience

[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics]Scaling law[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]010304 chemical physicsChemistryGeneral EngineeringInelastic collision010402 general chemistry01 natural sciencesDiatomic molecule0104 chemical sciencesClassical mechanics0103 physical sciencesPhysical and Theoretical ChemistryAtomic physicsComputingMilieux_MISCELLANEOUS
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A weakly-interacting many-body system of Rydberg polaritons based on electromagnetically induced transparency

2020

We proposed utilizing a medium with a high optical depth (OD) and a Rydberg state of low principal quantum number, $n$, to create a weakly-interacting many-body system of Rydberg polaritons, based on the effect of electromagnetically induced transparency (EIT). We experimentally verified the mean field approach to weakly-interacting Rydberg polaritons, and observed the phase shift and attenuation induced by the dipole-dipole interaction (DDI). The DDI-induced phase shift or attenuation can be viewed as a consequence of the elastic or inelastic collisions among the Rydberg polaritons. Using a weakly-interacting system, we further observed that a larger DDI strength caused a width of the mome…

Electromagnetically induced transparencyAtomic Physics (physics.atom-ph)QC1-999Inelastic collisionGeneral Physics and AstronomyFOS: Physical sciencesPhysics::OpticsAstrophysicsPhysics - Atomic Physicssymbols.namesakePrincipal quantum numberBose-Einstein condensation ; room-temperature ; single photons ; thermalization ; optics ; gasPolaritonPhysics::Atomic PhysicsQuantum informationPhysicsCondensed Matter::Quantum GasesQuantum PhysicsCondensed Matter::OtherPhysicsQB460-466Rydberg atomRydberg formulasymbolsRydberg stateAtomic physicsQuantum Physics (quant-ph)
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Polarization detection of trapped electrons via interaction with polarized atoms

1971

Electrons were trapped in an electrostatic quadrupole trap with superimposed homogeneous magnetic field. The electrons were polarized by spin exchange with a polarized atomic beam. The free trapped electron polarization was converted to a change in the electron translational energy via spin-dependent inelastic collisions with the atomic beam, and the electron translational temperature was monitored. Discussed are the development of this variation of the measurement technique, characteristics of electron storage, and the electron-polarized atom inelastic interaction as a function of electron temperature and time. The method has been applied to the detection of the (g-2) resonance of free, st…

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsSpin polarizationAtomElectron beam weldingCyclotron resonanceInelastic collisionElectron temperaturePhysics::Atomic PhysicsElectronAtomic physicsPolarization (waves)Zeitschrift für Physik A Hadrons and nuclei
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