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PARTICLE SIZE (in nm)
0
10
20
30
40
50
60
1.2
Q=2, q=1
Q=q=1
Q=1, q=2
1.0
ε
=5
0.8
0.6
0.4
0.2
0.0
0.2
0.4
0.6
0.8
1.0
PARTICLE SIZE (in units of l c )
Fig. 3.12 Influence of particle (ion) charge on double charging efficiency. Shown are the
suppression factors ".a/ as the function of particle size at different particle and ion charges Q
and q . Lower horizontal axis shows particle size in units of the Coulomb length l c
ˇe 2
D
momenta corresponding to the ion trajectories intersecting the particle surface. The
analysis becomes somewhat nontrivial because we consider the flux from a sphere
of finite radius R . In what follows we introduce the notation L a for the separating
angular momentum (its value depends on the ion energy).
3.6.1.1
Nonsingular Attraction
Let us begin by considering attractive nonsingular potentials j U.r/ j / r ˛ , ˛<2.
The function L 2 .r/ D 2mr 2 .E U.r// is shown schematically in Figs. 3.13
and 3.14 for E > 0and E < 0. It is seen that ions with L 2 <2m.E U.a//
are able to reach the particle surface. At E < 0 the situation changes; if
2mR 2 . j E j C j U.R/ j /<2ma 2 . j E j C j U.a/ j /, then the trajectories with
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