For any step , set . The Ornstein-Uhlenbeck transition distribution gives the exact update
using a fresh independent standard normal random variable for each interval. The update reproduces the joint probability distribution on the selected time grid. It can start from a fixed value or use Ornstein-Uhlenbeck stationary initialization. On an equally spaced grid it is an autoregressive process of order one after subtracting . Its stationary variance follows directly from .
For the stipulated example with , and the innovation variance is . Given , the next conditional expected value is about and the conditional standard deviation is about .
The Euler-Maruyama method instead approximates the same stochastic differential equation by
For its stationary variance solves , giving
At in the example, this is , about above the continuous model's stationary variance. If , this Euler recurrence has no finite stationary variance despite the stable continuous model. Exact transitions avoid this discretization error at sampled times; neither update alone determines the unresolved motion between samples.
Ornstein-Uhlenbeck process Created 2026-09-24 Updated 2026-10-14
An Ornstein-Uhlenbeck process combines mean reversion with continuing random fluctuations. In the scalar model, its stochastic differential equation is
where is a standard Brownian motion. The drift points towards : it is negative above and positive below it. The coefficient sets the speed of mean reversion, while sets the strength of the random forcing. We consider a fixed or normal initial value independent of future Brownian increments, giving a Gaussian process and a Markov process.
For a stipulated example, use , , and the fixed initial value , in arbitrary consistent state and time units. Then the expected value relaxes as and the variance grows as . At time one they are about and ; the limiting variance is one. The sample paths keep fluctuating even after the expected value is close to two. The Ornstein-Uhlenbeck transition distribution describes this evolving uncertainty; Ornstein-Uhlenbeck stationary initialization instead starts with that limiting normal distribution already in place.
A physical motivation is the velocity of a particle undergoing Brownian motion: linear drag removes a persistent initial velocity, while random forcing continually renews it. The original calculation gives a normal distribution for the velocity after subtracting its exponentially decaying initial contribution, with decay rate equal to the friction coefficient divided by the particle's mass.[ref] A position coordinate in an overdamped harmonic optical trap gives another interpretation of the same scalar equation, with for spring constant and drag coefficient . Its physical assumptions and connection to measurements are developed in thermal calibration of an optical trap.