TheoremComplete

Strong Markov Property for Brownian Motion

The strong Markov property states that Brownian motion "restarts" at a stopping time, independent of the past.


Statement

Theorem4.1Strong Markov property

Let Ο„\tau be a stopping time with P(Ο„<∞)=1\mathbb{P}(\tau < \infty) = 1. Define the shifted process B~t=BΟ„+tβˆ’BΟ„\tilde{B}_t = B_{\tau+t} - B_\tau for tβ‰₯0t \geq 0. Then (B~t)(\tilde{B}_t) is a Brownian motion independent of FΟ„=Οƒ(Bs:s≀τ)\mathcal{F}_\tau = \sigma(B_s : s \leq \tau).

This extends the ordinary Markov property (which holds at fixed times) to random times determined by the history of the process.

ExampleDistribution after hitting

Let Ο„a=inf⁑{t:Bt=a}\tau_a = \inf\{t : B_t = a\}. By the strong Markov property, (BΟ„a+tβˆ’a)(B_{\tau_a + t} - a) is a Brownian motion starting at 0, independent of the path before Ο„a\tau_a. This allows computation of hitting probabilities for multiple levels.


Applic ation: Gambler's ruin

ExampleHitting two levels

What is P(BΟ„=b∣B0=x)\mathbb{P}(B_\tau = b \mid B_0 = x), where Ο„=inf⁑{t:Bt∈{a,b}}\tau = \inf\{t : B_t \in \{a, b\}\} with a<x<ba < x < b? By the strong Markov property and martingale arguments, the probability is (xβˆ’a)/(bβˆ’a)(x-a)/(b-a).


Summary

The strong Markov property is fundamental to analyzing Brownian motion at random times, with applications to hitting times, exit problems, and optimal stopping.