Non-linear plasma wake growth of electron holes

An object's wake in a plasma with small Debye length that drifts across the magnetic field is subject to electrostatic electron instabilities. Such situations include, for example, the moon in the solar wind and probes in magnetized laboratory plasmas. The instability drive mechanism can equiva...

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Bibliographic Details
Main Authors: Hutchinson, Ian Horner (Contributor), Haakonsen, Christian Bernt (Contributor), Zhou, Chuteng (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Nuclear Science and Engineering (Contributor), Massachusetts Institute of Technology. Plasma Science and Fusion Center (Contributor)
Format: Article
Language:English
Published: American Institute of Physics (AIP), 2016-10-28T16:05:30Z.
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Online Access:Get fulltext
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001 105129
042 |a dc 
100 1 0 |a Hutchinson, Ian Horner  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Nuclear Science and Engineering  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Plasma Science and Fusion Center  |e contributor 
100 1 0 |a Hutchinson, Ian Horner  |e contributor 
100 1 0 |a Haakonsen, Christian Bernt  |e contributor 
100 1 0 |a Zhou, Chuteng  |e contributor 
700 1 0 |a Haakonsen, Christian Bernt  |e author 
700 1 0 |a Zhou, Chuteng  |e author 
245 0 0 |a Non-linear plasma wake growth of electron holes 
260 |b American Institute of Physics (AIP),   |c 2016-10-28T16:05:30Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/105129 
520 |a An object's wake in a plasma with small Debye length that drifts across the magnetic field is subject to electrostatic electron instabilities. Such situations include, for example, the moon in the solar wind and probes in magnetized laboratory plasmas. The instability drive mechanism can equivalently be considered drift down the potential-energy gradient or drift up the density-gradient. The gradients arise because the plasma wake has a region of depressed density and electrostatic potential into which ions are attracted along the field. The non-linear consequences of the instability are analysed in this paper. At physical ratios of electron to ion mass, neither linear nor quasilinear treatment can explain the observation of large-amplitude perturbations that disrupt the ion streams well before they become ion-ion unstable. We show here, however, that electron holes, once formed, continue to grow, driven by the drift mechanism, and if they remain in the wake may reach a maximum non-linearly stable size, beyond which their uncontrolled growth disrupts the ions. The hole growth calculations provide a quantitative prediction of hole profile and size evolution. Hole growth appears to explain the observations of recent particle-in-cell simulations. 
520 |a National Science Foundation (U.S.) (Basic Plasma Science Partnership under Grant No. DE-SC0010491) 
520 |a United States. Department of Energy. (Basic Plasma Science Partnership under Grant No. DE-SC0010491) 
546 |a en_US 
655 7 |a Article 
773 |t Physics of Plasmas