
140 Compact Plasma and Focused Ion Beams
considering the change of T
e
. Solid lines in Figure 8.8 labeled as 1, 2 show
the result of numerical simulation of the rst and second parts of the decay
at 0.24 and 0.58 Torr, respectively. The decay at the lower p could be tted
rather well. The higher p exhibited a splitting with a rise in the ion density.
The reason for the splitting is not known, and one possibility could be the
generation of NO
x
ions (e.g., NO
+
,
2
etc.), which have not been taken into
consideration in our model.
The experimental data tted with curves 1 and 2 represent the following
dimensionless parameter values. Sufxes I a ...