IOP PUBLISHING JOURNAL OF PHYSICS D: APPLIED PHYSICS
J. Phys. D: Appl. Phys. 41 (2008) 015210 (9pp) doi:10.1088/0022-3727/41/1/015210
Self-consistent spatio-temporal simulation
of pulsed microwave discharge
Z Bonaventura, D Trunec, M Meˇ sko, P Vaˇ sina and V Kudrle
Department of Physical Electronics, Faculty of Science, Masaryk University, Kotl´ aˇ rsk´ a 2, 611 37 Brno,
Czech Republic
E-mail: zbona@physics.muni.cz
Received 24 April 2007, in final form 17 October 2007
Published 19 December 2007
Online at stacks.iop.org/JPhysD/41/015210
Abstract
A spatio-temporal theoretical model of pulsed microwave discharge was developed. This
model is based on the macroscopic continuity equation for electrons and on the wave equation
for an electromagnetic wave passing through the discharge plasma. These equations were
solved together and in a self-consistent manner. For simplicity, the continuity equation was
solved in one dimension only and the electromagnetic wave was assumed to be plane and
transversal. Both equations were solved numerically and the spatio-temporal dependences of
electron concentration and the amplitude of the microwave electric field were obtained. It was
found that the discharge development depends, significantly, on the initial spatial distribution
of electron concentration. Two different cases were studied: the discharge development during
the first microwave pulse only and after several successive pulses. The calculations were
performed particularly for the discharge in nitrogen. The results were compared with
experimental data from our previous work.
M Animations of the time development of figures 7, 8 and 9 are available in the online edition
at http://stacks.iop.org/JPhysD/41/015210
1. Introduction
Pulsed microwave discharges have already been studied by our
group both experimentally and theoretically. In the experiment
[1] the time dependences of electron concentration, transmitted
microwave power and selected nitrogen band intensities were
measured for pulsed microwave discharge in nitrogen. The
electron distribution function and macroscopic parameters
(mean energy, ionization and diffusion coefficients, etc) were
obtained from the solution of the Boltzmann equation [2, 3]
for the conditions corresponding to the experiment. It was
found that microwave power is significantly absorbed and/or
reflected by the discharge plasma. To take into account
this effect, it is necessary to solve the wave equation for
the electromagnetic wave passing through the plasma. The
influence of plasma on the wave propagation is described
by complex conductivity. Solving the wave equation, the
spatial distribution of electric field strength amplitude, E
0
, is
obtained and this quantity is used to determine the ionization
and diffusion coefficients and the complex conductivity. These
coefficients are dependent on E
0
. The time development
of electron concentration is described by the continuity
equation with corresponding source and loss terms. Since
the electromagnetic wave influences the electron concentration
and the propagation of the wave is influenced by the electron
concentration, it is necessary to solve the wave equation and
the continuity equation together in a self-consistent manner.
During our experimental work [1] several interesting
questions arose. Where and when exactly is the discharge
ignited? Is the observed stratification caused by the wave
reflection from plasma? The model presented in this paper
was developed in particular to answer these questions and
consequently to gain a better understanding of temporal
behaviour in this type of plasma. For simplicity, the
calculations were performed in one spatial dimension only
and the electromagnetic wave was assumed to be plane and
transversal.
Pulsed microwave discharge in nitrogen was studied
experimentally and theoretically by Baeva and co-workers
[4, 5] and Repsilber et al [6]. However, the theoretical
models in these studies were not self-consistent; they were
based on the numerical solution of the Boltzmann equation
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