Significant progress has been achieved during the last decade in our k
nowledge and understanding of the optical potential between two light
heavy-ions. This has mostly been a consequence of the measurement of a
ccurate and extensive elastic differential cross sections. Some of the
se data, covering over eight orders of magnitude in cross section, ext
end to sufficiently large scattering angles that they show remarkable
refractive effects which remind one of features of the scattering of a
lpha particles by nuclei that have been known since the work of Goldbe
rg some twenty years ago. Refractive effects, particularly nuclear rai
nbows, are evident in C-12 + C-12 and O-16 + O-16 angular distribution
s at bombarding energies between 6 and 100 MeV per nucleon. Their angu
lar location and cross section have led to the determination of the gr
oss features of the local optical potentials and in many cases have re
moved ambiguities in the depths of the real parts of the potentials. T
he resulting phenomenological potentials are strongly attractive (''de
ep''), with relatively weak absorption, and depend upon the bombarding
energy. The optical model potential for such heavy-ions is no longer
simply a way to parameterize scattering data (or perhaps just one of m
any ways). Ambiguities have been resolved, and a good understanding of
the theoretical basis of its features has been attained. The folding
model is central to this understanding, coupled with increased insight
into the nature of realistic effective nucleon-nucleon interactions.
This Report reviews the experimental evidence, its interpretation, and
what we have learnt from it. Much of the interpretation becomes espec
ially transparent when couched in the language of semiclassical scatte
ring theory. We summarize this language, as well as the basic features
of the theory of the optical model.