
6 Compact Plasma and Focused Ion Beams
attracted to the vicinity of an electron and shield its electrostatic
eld from the rest of the plasma.
Therefore, charged particles arrange themselves to shield all elec-
trostatic elds within a distance of the approximate Debye’s length.
The electrostatic potential of an isolated particle of charge q is
φ
= q/r.
Because of the shielding effect, the potential in the vicinity of the
charged particle in a plasma is altered and therefore the potential of
a charge at rest in a plasma is given by
j
l
=
−
e
r
D
/
.
(1.8)
In other words, in the neighborhood of any surface inside the
plasma, there is a lay ...