1984
DOI: 10.1088/0031-8949/30/1/015
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Electron Phase Space Holes as Localized BGK Solutions

Abstract: The main properties of the electron Bemstein-Greene-Kruskal solitary waves (electron holes) a e investigated prescribing the model potential shapes. The analytical expressions for the trapped particles distributions and the width dependence on the amplitude are obtained following the classic BGK method. It is shown that in a stationary kinetic consideration there is no limitation on the hole Mach number. Such a limitation arises only from the conditions of the BGK wave stability. The temporal evolution of the … Show more

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Cited by 94 publications
(90 citation statements)
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“…The pulse has a symmetric positive potential with dipolar electric field and a charge density which is positive at the center and negative near the edges. These properties are consistent with a Bernstein-Greene-Kruskal electron hole [1]. The shaded area corresponds to a theoretically inaccessible region [11].…”
Section: Electrostatic Solitary Structures Identified Assupporting
confidence: 75%
See 1 more Smart Citation
“…The pulse has a symmetric positive potential with dipolar electric field and a charge density which is positive at the center and negative near the edges. These properties are consistent with a Bernstein-Greene-Kruskal electron hole [1]. The shaded area corresponds to a theoretically inaccessible region [11].…”
Section: Electrostatic Solitary Structures Identified Assupporting
confidence: 75%
“…In particular the plasma in which the solitary waves propagate is likely warmer due to the interaction with the beam, making the structure velocities closer to the actual thermal speed. Indeed it was predicted that electron holes faster than 2v T e are unstable [1] and are therefore unlikely to be observed. Normalization questions apart, electron hole sizes significantly larger than 位 De are theoretically allowed.…”
Section: Electrostatic Solitary Structures Identified Asmentioning
confidence: 99%
“…Electron phase space holes have been long studied as examples of nonlinear solitary structures, either as solutions of the unmagnetized Vlasov-Maxwell system (BGK waves), 12 the Vlasov-Poisson system, 13 or using fluid models. 14,15 These structures depend for their existence on particle trapping in the electrostatic potential of the wave. A model of magnetic structure associated with electron phase space holes has been proposed by Treumann and Baumjohann, 16 in which an azimuthal electron current is driven by the E 脗 B drift, enhancing the magnetic field at the center and reducing it outside.…”
Section: Introductionmentioning
confidence: 99%
“…The trapped particles play crucial roles in these models (Bernstein et al, 1957;Turikov, 1984). The waveform observations by the plasma wave instrument on board the Geotail spacecraft have shown that broad band electrostatic noise (BEN) consists of a series of bipolar solitary pulses .…”
Section: Bgk Modes/phase Space Holesmentioning
confidence: 99%