| Model 1 | For the first model, for each input electron the number of additional electrons generated by impact ionisation within the gain stage was selected from a Poisson distribution. This corresponds to the case where impact ionisation is an instantaneous process, and an input electron can generate multiple charge carriers within a single gain stage. Impact ionisation events triggered by secondary electrons generated within that gain stage were not considered. |
| Model 2 | For the second model, a maximum of one additional electron could be generated through impact ionisation within one gain stage. This corresponds to the case where the generation of additional electrons by impact ionisation cannot occur twice within the time taken to transfer the charge from one gain stage to the next. |
It is unlikely that either model perfectly describes the real operation of a gain stage, but the models considered here cover a reasonably broad spectrum of possible properties.
Bob Tubbs 2003-11-14