For standard three-dimensional Brownian motion started at with ,
The harmonic function gives a bounded stopped martingale in the annulus, so the optional stopping theorem gives the formula. Taking yields for . This limit uses path continuity on the finite interval before a hit, rather than assuming transience to prove transience.
Define the stopped martingale
It is nonnegative: before the first visit to , the nearest-neighbour random walk is at most , and afterwards the stopped position is . Each is integrable, with . Moreover
The indicator is -measurable and the increment has conditional mean zero, so is a martingale with .
Part (a) shows almost surely, so every such path eventually has . Thus almost surely. But for every , so there is no convergence in L1. Any possible L1 convergence limit would agree with the almost sure limit. This is a nonnegative martingale with almost sure convergence but no convergence in L1, and hence it is not uniformly integrable.
The bounded optional stopping theorem gives . Decompose the difference from the terminal value:
Consequently
The first term tends to zero by hypothesis. The second tends to zero by the dominated convergence theorem, because is integrable and is finite with probability one. Thus the stopped martingale converges to with convergence in L1, which permits passage of expectations to the limit:
The explicit tail condition supplies exactly the missing control for an unbounded stopping time.
Write and . Since is a stopping time, . The Tonelli theorem, conditional expectation, and (c)'s tail-sum formula for expectation yield
Thus is an integrable random variable. Since , telescoping gives and . The dominated convergence theorem gives , so (b) gives uniform integrability of the stopped martingale.
The optional stopping theorem at the bounded stopping time gives . Passing to the limit using the convergence in L1 proved in (b),
One can also pass directly by the dominated convergence theorem, since .
Put . By independence of the two Brownian motions, is a standard Brownian motion: its independent increments have the normal distribution with variance equal to elapsed time. The stopping time is the first time hits or .
To justify finiteness without presupposing the desired hitting probability, each unit-time increment of has the normal distribution . An increment of absolute value greater than forces exit from if the path was inside at its start. These independent increments give , where . Hence almost surely.
The stopped martingale lies in . The optional stopping theorem at gives , and the bounded convergence theorem gives . Writing , path continuity gives . Therefore, as in Brownian exit from an interval,
The increments of satisfy
Since , the indicator is predictable. Part (a), applied to this bounded integrand, shows that is a martingale. Equivalently, this is the stopped martingale theorem.
For a simple symmetric random walk, the infinite mean first passage of a simple symmetric random walk gives a finite almost sure first passage to . The stopped martingale is nonnegative and eventually zero almost surely. Nevertheless for every , so it has almost sure convergence but no convergence in L1. It is therefore not uniformly integrable. Before absorption the nearest-neighbour walk is at most zero, ensuring nonnegativity.