The concept of a light ion beam driver for Inertial Fusion Energy (IFE) is
based on multi-terawatt, multi-megavolt pulsed power generators, two-stage
ion acceleration and charge neutralised transport. In this paper we discuss
the present status for each of these components and identify the main issu
es for research. Only modest extrapolations from presently available techno
logies seem necessary for the high voltage pulse generator. The greatest ch
allenge of this approach is the accelerator, which will consist of two stag
es, the injector and the post-accelerator. Large progress has been made in
understanding the physical phenomena occurring in the injector gap. This pr
ogress has become possible by new sophisticated diagnostics that allowed de
tailed temporally and spatially resolved measurements of field and particle
densities in the acceleration gap and by relativistic fully electromagneti
c PIG-simulation tools, that stimulated analytic models. The conclusions dr
awn from these studies, namely limiting the ion current density to small en
hancements to reduce the beam divergence need still to be verified experime
ntally. Systematic experimental research on post-acceleration at high power
and voltage must aim at a complete understanding of instabilities coupling
from the injector to the post-accelerator and at limiting voltages and bar
riers for the extraction of unwanted ions from plasmas at the injection sid
e. Ultimately the light ion approach requires rep-rateable large area ion s
ources with ion masses greater than 1 and particle energies around 30 MeV.
Although different cleaning protocols were able to reduce the amount of par
asitic ions in the Li beam from a LiF field emission source the achievement
s are still insufficient. A field of common interest between light and heav
y ion beam driven fusion is beam transport from the accelerator to the targ
et. Supposedly the most favourable concept for both approaches is self-pinc
hed transport. Experimental evidence for self-pinched transport has recentl
y been achieved in an experiment at NRL. Further experiments are needed to
determine the dynamics and magnitude of net current formation, the efficien
cy of transport and the effect of bunching. (C) 2001 Elsevier Science B.V.
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