
278 Compact Plasma and Focused Ion Beams
start of the pulse, t = 0), depending upon the pressure, which is in conformity
to earlier experimental results with shorter-duration pulses.
From the electron plasma oscillations, as shown in the inset of Figure 17.2a,
an exponential decay factor
α
is obtained by considering the peak ampli-
tude of the waves. Figure 17.3 shows that
α
increases with pressure, indicat-
ing that electron–neutral collisions play an important role in damping these
waves. The growth rate
β
of the electron current after the end of the plasma
wave is estimated to be of the order of 10
5
s
−1
, as shown in Figure 17.3, and
increases ...