1982
DOI: 10.1029/ja087ia09p07445
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Particle pitch angle diffusion due to nonadiabatic effects in the plasma sheet

Abstract: In order to understand certain aspects of the plasma sheet dynamics, a numerical study of the nonadiabatic behavior of particles in a model field geometry is performed. The particle's magnetic moment as a function of time is calculated for various initial parameters, corresponding to various particle energies and degrees of field curvature. It is shown that the magnetic moment changes as the particle passes through the plasma sheet and that the magnitude of the change is related to the curvature of the field a… Show more

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Cited by 69 publications
(39 citation statements)
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“…On the contrary, ions in the supra-thermal energy regime are expected to behave in a non-adiabatic manner and hence their pitch angle distribution looses its anisotropic features. This follows from the fact that ions are subjected to a continuous isotropization because of random changes in the magnetic moment each time they cross the middle of the plasma sheet, experiencing a spatial variation of the magnetic field on the order of their gyroradius (collisionless pitch angle scattering) (Gray and Lee, 1982). The above mechanism further forces energetic ions to execute Speiser orbits and as a result, the ions return to the current sheet in a location much closer to the Earth than the one from which they were ejected.…”
Section: Particle Energization and Non-adiabaticitymentioning
confidence: 99%
“…On the contrary, ions in the supra-thermal energy regime are expected to behave in a non-adiabatic manner and hence their pitch angle distribution looses its anisotropic features. This follows from the fact that ions are subjected to a continuous isotropization because of random changes in the magnetic moment each time they cross the middle of the plasma sheet, experiencing a spatial variation of the magnetic field on the order of their gyroradius (collisionless pitch angle scattering) (Gray and Lee, 1982). The above mechanism further forces energetic ions to execute Speiser orbits and as a result, the ions return to the current sheet in a location much closer to the Earth than the one from which they were ejected.…”
Section: Particle Energization and Non-adiabaticitymentioning
confidence: 99%
“…7(a) and 7(b)). This irreversibility is due to the non-adiabaticity in the particle behavior: At the bottom panels of Figs the ratio, (particle gyroradius p)/(field curvature radius Rc) as a measure of non-adiabaticity (Gray and Lee, 1982). Since these ratios become of -1 after the type-I energization, the particle magnetic moments are not conserved.…”
Section: Traveling Of the Energized Particles Around A Plasmoidmentioning
confidence: 99%
“…These studies show the complexity and importance of the particle motion near the neutral sheet, where the adiabaticity of the particle motion is easily violated. Calculations of test particle trajectories in stationary neutral sheet were also studied by several authors (Speiser, 1965;Sonnerup, 1971;Wagner et al, 1979;Gray and Lee, 1982). Wagner et al have classified the particle orbits into adiabatic, transitional, and non-adiabatic case, according to the field geometry.…”
Section: Introductionmentioning
confidence: 99%
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“…This simplification comes directly from our assumption about strong localization of a magnetic field perturbation, i.e., the scale is substantially smaller than the scale of dipole field inhomogeneity ∼ LR E . This model is widely used for investigations of charged particle scattering due to nonadiabatic motion [e.g., Gray and Lee, 1982;Birmingham, 1984;Delcourt et al, 1995]. The Hamiltonian of relativistic electrons with the rest mass m and the charge −e in this magnetic field has the following form:…”
Section: Model Of the Electron Scatteringmentioning
confidence: 99%