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Trapping and ionization by plasma electrons in IFR beam propagation in the presence of an axial field

Conference ·
OSTI ID:6854336

As a relativistic electron beam propagates into a plasma channel in the ion-focused regime (IFR), the plasma electrons are ejected under the influence of the beam electrostatic field. If there is an axial magnetic field, it is possible for the plasma electrons to be trapped on orbits within the drift tube radius. These trapped electrons are highly energetic (compared to ionization energies) and thus for long pulse beams it is possible that the channel density would vary as a function of time due to ionization by the trapped electrons. It is also possible that plasma electrons trapped in the vicinity of the beam would cause electron-electron instabilities. Trapping and ionization by plasma electrons is considered in this paper. First, we derive a transcendental equation for the electron trapping radius in terms of the beam parameters and the external field. We then find an expression for the time-averaged plasma electron density profile in the presence of the relativistic beam. Finally, we estimate the ionization rate by these electrons. In the following analysis, it is assumed that only the beam electrostatic forces act on the plasma electrons; that is, forces due to channel ions and electrons are neglected. This limits the applicability of the analysis to problems with small neutralization fractions. We also neglect electrodynamic effects. 1 ref., 2 figs.

Research Organization:
Sandia National Labs., Albuquerque, NM (USA)
DOE Contract Number:
AC04-76DP00789
OSTI ID:
6854336
Report Number(s):
SAND-88-2414C; CONF-8809149-2; ON: DE89000454
Country of Publication:
United States
Language:
English