This paper discusses the information about a device that is contained
in the experimental heavy ion cross section curve. The width and shape
of the curve are shown to be determined by intra-cell variations of c
harge collection, not by cell to cell variations. If we assume that th
ere is a unique charge that must appear on the transistor terminal, th
en the cross section may be described in terms of variation of effecti
ve charge collection depth across the device. Contours of constant cha
rge collection can be determined from the parameters that describe the
cross section curve. The effects of diffusion can be distinguished fr
om the other charge collection processes.