Rr. Arslanbekov et al., Electron-distribution-function cutoff mechanism in a low-pressure afterglow plasma - art. no. 016401, PHYS REV E, 6401(1), 2001, pp. 6401
A model is developed for self-consistent simulations of transient phenomena
in a low-pressure afterglow plasma. The model is based on the nonlocal app
roach which allows a kinetic description of the plasma decay under nonquasi
stationary conditions. Such conditions arise when collisions (mainly electr
on-electron) are not sufficient for the electron distribution function (EDF
) to follow changes in the self-consistent electric fields and the ion dens
ity once the power is turned off. As a result, collisions cannot provide th
e electron and ion particle balance by allowing electrons to flow out of th
e potential well. A cutoff mechanism is suggested that provides such a bala
nce during the transient period-from the glow, stationary plasma to the qua
sistationary, afterglow plasma. This mechanism is essential for determining
correctly the self-consistent wall potential (and hence the energy of ions
impinging upon the wall surface) and other parameters, such as diffusion c
ooling, which is the most important cooling mechanism at low pressures. The
se phenomena are modeled using the time-dependent nonlocal electron Boltzma
nn equation with a nonlinear electron-electron collision operator. A numeri
cal treatment is made by extending Rockwood's method for finite-difference
discretization of this operator in the total energy formulation. The model
calculates self-consistently the temporal evolution of the nonlocal EDF and
the electric potentials in the plasma and the wall sheath. Strongly non-Ma
xwellian EDF's are predicted and it is observed that, depending on plasma c
onditions, the transient period maybe rather long, of order of the ambipola
r diffusion time, lower pressures resulting in longer transient times. The
proposed approach can be applied to model self-consistently pulsed plasmas
during both the power-on and power-off periods, including the breakdown per
iod.