For every finite collection of positive times, is a linear transformation of the corresponding values of , so is a centered Gaussian process. If , thenThus has the covariance of Brownian motion.
Its paths are continuous for . As , put . The given almost-sure limit givesThe Gaussian-process characterization of Brownian motion now proves the time inversion of Brownian motion:
Use the time-inverted Brownian motion . For , set . ThenAs corresponds exactly to , and the inequality at is automatic because , this is the pathwise identitySince and have the same law by time inversion of Brownian motion,
Let and . Split the crossing event according to its endpoint:Under the Cameron-Martin theorem for a linear drift, the law of relative to standard Wiener measure has endpoint densityOn paths that cross and end at , the Brownian reflection principle reflects the path after its first hit of and changes the endpoint to . Under this reflection the density becomesThe remaining exponential is the Cameron--Martin density for drift . Thereforewhere the last equality uses the symmetry of the normal distribution. Subtracting the crossing probability from one givesEquivalently, in terms of the standard normal distribution function,This is the finite-horizon maximum of Brownian motion with negative drift formula.
By continuity of Brownian motion, the event that the last strict crossing of occurs by time isApply part (b) with and interchanged and its time parameter replaced by . This turns the right-hand side intoPart (c), now with drift , barrier , and horizon , givesThis is the distribution function of the last passage time above a level for Brownian motion with negative drift. Taking givesthe probability that the negatively drifted Brownian path never exceeds , consistent with the infinite-horizon crossing probability for Brownian motion with negative drift.
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