Key points are not available for this paper at this time.
yield the recurrence relation p(a + I)eis g(a; a + 1) = 1-q(a + 1)el8g(a + 1; a + 2) (6.4) T. Discussion.-The foregoing techniques can be extended to treat the case where there is a general distribution of jumps at each stage, and the case where we introduce time dependence by requiring the probability that the particle emerge at a on or before a given time T.These matters, as well as those mentioned in Section 1, will be discussed in subsequent papers.
Raoul Bott (Tue,) studied this question.