TheoremComplete

Lévy's Characterization of Brownian Motion

Lévy's theorem provides a characterization of Brownian motion via the martingale property and quadratic variation.


Statement

Theorem4.1Lévy's characterization

A continuous process (Mt)t0(M_t)_{t \geq 0} with M0=0M_0 = 0 is a Brownian motion if and only if:

  1. (Mt)(M_t) is a martingale.
  2. [M]t=t[M]_t = t (quadratic variation equals tt).

This theorem is powerful: to verify a process is Brownian, we need only check the martingale property and quadratic variation, not the full Gaussian increment structure.

ExampleTime-changed Brownian motion

If (Bt)(B_t) is Brownian motion and (At)(A_t) is a continuous increasing process with A0=0A_0 = 0, define Mt=BAtM_t = B_{A_t}. If At=tA_t = t (the identity), then MtM_t is Brownian. More generally, MtM_t is a time-changed Brownian motion.


Application: Donsker's invariance principle

Theorem4.2Donsker's theorem

Let X1,X2,X_1, X_2, \ldots be i.i.d. with mean 0 and variance 1. Define the random walk scaled to continuous time:

Wn(t)=1ni=1ntXi.W_n(t) = \frac{1}{\sqrt{n}} \sum_{i=1}^{\lfloor nt \rfloor} X_i.

Then WnBW_n \Rightarrow B in distribution (in the space of continuous functions), where BB is Brownian motion.

Donsker's theorem shows that Brownian motion is the universal scaling limit of random walks.


Summary

Lévy's characterization simplifies verification of Brownian motion and provides a foundation for stochastic calculus, where processes are often constructed as martingales with specified quadratic variation.