Abstract
Two counterpropagating cool and equally dense electron beams are modeled with particle-in-cell simulations. The electron beam filamentation instability is examined in one spatial dimension, which is an approximation for a quasiplanar filament boundary. It is confirmed that the force on the electrons imposed by the electrostatic field, which develops during the nonlinear stage of the instability, oscillates around a mean value that equals the magnetic pressure gradient force. The forces acting on the electrons due to the electrostatic and the magnetic field have a similar strength. The electrostatic field reduces the confining force close to the stable equilibrium of each filament and increases it farther away, limiting the peak density. The confining time-averaged total potential permits an overlap of current filaments with an opposite flow direction.
Original language | English |
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Article number | 074502 |
Pages (from-to) | 074502-074502-4 |
Number of pages | 74499 |
Journal | Physics of Plasmas |
Volume | 16 |
Issue number | 7 |
Publication status | Published - Jul 2009 |
ASJC Scopus subject areas
- Condensed Matter Physics