Reflection principle (Wiener process)

Summary

In the theory of probability for stochastic processes, the reflection principle for a Wiener process states that if the path of a Wiener process f(t) reaches a value f(s) = a at time t = s, then the subsequent path after time s has the same distribution as the reflection of the subsequent path about the value a.[1] More formally, the reflection principle refers to a lemma concerning the distribution of the supremum of the Wiener process, or Brownian motion. The result relates the distribution of the supremum of Brownian motion up to time t to the distribution of the process at time t. It is a corollary of the strong Markov property of Brownian motion.

Simulation of Wiener process (black curve). When the process reaches the crossing point at a=50 at t3000, both the original process and its reflection (red curve) about the a=50 line (blue line) are shown. After the crossing point, both black and red curves have the same distribution.

Statement edit

If   is a Wiener process, and   is a threshold (also called a crossing point), then the lemma states:

 

Assuming   , due to the continuity of Wiener processes, each path (one sampled realization) of Wiener process on   which finishes at or above value/level/threshold/crossing point   the time   (   ) must have crossed (reached) a threshold   (   ) at some earlier time   for the first time . (It can cross level   multiple times on the interval  , we take the earliest.)

For every such path, you can define another path   on   that is reflected or vertically flipped on the sub-interval   symmetrically around level   from the original path. These reflected paths are also samples of the Wiener process reaching value   on the interval  , but finish below  . Thus, of all the paths that reach   on the interval  , half will finish below  , and half will finish above. Hence, the probability of finishing above   is half that of reaching  .

In a stronger form, the reflection principle says that if   is a stopping time then the reflection of the Wiener process starting at  , denoted  , is also a Wiener process, where:

 

and the indicator function   and  is defined similarly. The stronger form implies the original lemma by choosing  .

Proof edit

The earliest stopping time for reaching crossing point a,  , is an almost surely bounded stopping time. Then we can apply the strong Markov property to deduce that a relative path subsequent to  , given by  , is also simple Brownian motion independent of  . Then the probability distribution for the last time   is at or above the threshold   in the time interval   can be decomposed as

 .

By the tower property for conditional expectations, the second term reduces to:

 

since   is a standard Brownian motion independent of   and has probability   of being less than  . The proof of the lemma is completed by substituting this into the second line of the first equation.[2]

 .

Consequences edit

The reflection principle is often used to simplify distributional properties of Brownian motion. Considering Brownian motion on the restricted interval   then the reflection principle allows us to prove that the location of the maxima  , satisfying  , has the arcsine distribution. This is one of the Lévy arcsine laws.[3]

References edit

  1. ^ Jacobs, Kurt (2010). Stochastic Processes for Physicists. Cambridge University Press. pp. 57–59. ISBN 9781139486798.
  2. ^ Mörters, P.; Peres, Y. (2010) Brownian Motion, CUP. ISBN 978-0-521-76018-8
  3. ^ Lévy, Paul (1940). "Sur certains processus stochastiques homogènes". Compositio Mathematica. 7: 283–339. Retrieved 15 February 2013.