Plasma instabilities have been studied in low-pressure inductive processing
discharges with SF6 and Ar/SF6 mixtures, i.e. attaching gases. Oscillation
s are seen in charged particle density, electron temperature and plasma pot
ential using electrostatic probe and optical emission measurements. For SF6
, instability onset in pressure and driving power has been explored for gas
pressures between 2.5 and 100 mTorr and absorbed powers between 150 and 90
0 W. For pressures above 20 mTorr, increasing power is required to obtain t
he instability with increasing pressure, with the frequency of the instabil
ity increasing with pressure, mainly lying between 1 and 100 kHz. For Ar/SF
6 mixtures, we observe a similar low power transition, with an upper transi
tion to a stable inductive mode. The instability windows become smaller as
the argon partial pressure increases. For Ar/SF6 mixtures, we observe a sig
nificant effect of the matching network. We improve a previously developed
volume-averaged (global) model to describe the instability. We consider a c
ylindrical discharge containing time varying electrons, positive ions, nega
tive ions, and time invariant excited states. The driving power is applied
to the discharge through a conventional L-type capacitive matching network,
and we use realistic models for the inductive and capacitive energy deposi
tion. The particle and energy balance equations are integrated, considering
quasi-neutrality in the plasma volume and charge balance at the walls, to
produce the dynamical behaviour. As pressure or power is varied to cross a
threshold, the instability is born at a Hopf bifurcation, with relaxation o
scillations between higher and lower density states. The model qualitativel
y agrees with experimental observations, and also shows a significant influ
ence of the matching network.