The Wiener process: continuous-time random motion with fundamental applications
A standard Brownian motion (Wiener process) is a stochastic process with:
Key Properties:
For , the probability that Brownian motion reaches level before time is:
This is used to calculate hitting time probabilities: .
Geometric Brownian motion models stock prices:
where is the drift, is the volatility, and is standard Brownian motion.
Problem:
Find for standard Brownian motion.
Solution:
.
Problem:
Find where is the hitting time of level 2.
Solution:
Using reflection principle: .
Problem:
For with and , find the distribution of .
Solution:
.
Since , we have .
Norbert Wiener provided the first mathematical construction of Brownian motion in 1923, proving its existence rigorously. While Robert Brown observed the phenomenon in 1827 and Einstein explained it physically in 1905, Wiener's mathematical formulation is why it's also called the Wiener process.
Sample path continuity means that for every outcome ω, the function t → B(t,ω) is continuous (no jumps). This is remarkable because even though the process has continuous paths, those paths are nowhere differentiable—they're infinitely rough at all scales.
The reflection principle says: if Brownian motion hits level 'a' before time t, and we reflect the path about 'a' afterwards, we get the same distribution. Mathematically, P(max B(s) ≥ a) = 2P(B(t) ≥ a). This symmetry is powerful for calculating hitting time and maximum distributions.
For any c>0, {B(ct)/√c} has the same distribution as {B(t)}. This means zooming in or out looks statistically the same—a fractal property. It's why Brownian motion appears equally rough at all time scales. The exponent H=1/2 is called the Hurst parameter.
Standard Brownian motion B(t) can be negative (symmetric around 0). Geometric Brownian motion S(t)=S₀e^{μt+σB(t)} is always positive, making it suitable for stock prices. The 'geometric' means percentage changes (not absolute) are normally distributed.