Chapter 14: Wiener Processes and Itô's Lemma
5 min readThe Markov Property
A Markov process is one where only the current value of a variable is relevant for predicting the future — the path history is irrelevant. Stock prices are generally assumed to follow Markov processes, consistent with the weak form of market efficiency.
Continuous-Time Stochastic Processes
Wiener Process (Brownian Motion)
A Wiener process z(t)z(t) has two properties:
- Δz=εΔt\Delta z = \varepsilon \sqrt{\Delta t}, where ε∼N(0,1)\varepsilon \sim N(0, 1)
- The values of Δz\Delta z for any two non-overlapping intervals are independent
This means:
- E[Δz]=0E[\Delta z] = 0
- Var(Δz)=Δt\text{Var}(\Delta z) = \Delta t
- Var(z(T)−z(0))=T\text{Var}(z(T) - z(0)) = T (variance grows linearly with time)
Generalized Wiener Process
dx=a dt+b dzdx = a \, dt + b \, dz
where:
- aa = drift rate (expected change per unit time)
- bb = variance rate (standard deviation of change per unit time)
Δx=a⋅Δt+b⋅εΔt\Delta x = a \cdot \Delta t + b \cdot \varepsilon \sqrt{\Delta t}
Itô Process
Allows aa and bb to depend on xx and tt:
dx=a(x,t) dt+b(x,t) dzdx = a(x, t) \, dt + b(x, t) \, dz
The Process for a Stock Price
Stock prices follow geometric Brownian motion:
dS=μS dt+σS dzdS = \mu S \, dt + \sigma S \, dz
or equivalently:
dSS=μ dt+σ dz\frac{dS}{S} = \mu \, dt + \sigma \, dz
- μ\mu = expected rate of return (annualized)
- σ\sigma = volatility (annualized standard deviation of returns)
- In a risk-neutral world, μ\mu = rr (the risk-free rate)
Discrete-time approximation:
ΔSS∼N(μ Δt,σ2Δt)\frac{\Delta S}{S} \sim N(\mu \, \Delta t, \sigma^2 \Delta t)
Itô's Lemma
Itô's lemma is the stochastic calculus equivalent of the chain rule. If xx follows an Itô process and G(x,t)G(x, t) is a function of xx and tt:
dG=(∂G∂xa+∂G∂t+12∂2G∂x2b2)dt+∂G∂xb dzdG = \left(\frac{\partial G}{\partial x} a + \frac{\partial G}{\partial t} + \frac{1}{2} \frac{\partial^2 G}{\partial x^2} b^2\right) dt + \frac{\partial G}{\partial x} b \, dz
Applied to stock prices (dS=μSdt+σSdzdS = \mu S dt + \sigma S dz):
dG=(∂G∂SμS+∂G∂t+12∂2G∂S2σ2S2)dt+∂G∂SσS dzdG = \left(\frac{\partial G}{\partial S} \mu S + \frac{\partial G}{\partial t} + \frac{1}{2} \frac{\partial^2 G}{\partial S^2} \sigma^2 S^2\right) dt + \frac{\partial G}{\partial S} \sigma S \, dz
For G=lnSG = \ln S (a commonly used transformation):
d(lnS)=(μ−σ22)dt+σ dzd(\ln S) = \left(\mu - \frac{\sigma^2}{2}\right) dt + \sigma \, dz
This implies that lnS\ln S follows a generalized Wiener process with drift μ−σ2/2\mu - \sigma^2/2 and variance rate σ2\sigma^2.
The Lognormal Property
From Itô's lemma applied to lnS\ln S, we conclude:
lnST−lnS0∼N[(μ−σ22)T,σ2T]\ln S_T - \ln S_0 \sim N\left[\left(\mu - \frac{\sigma^2}{2}\right)T, \sigma^2 T\right]
or:
lnST∼N[lnS0+(μ−σ22)T,σ2T]\ln S_T \sim N\left[\ln S_0 + \left(\mu - \frac{\sigma^2}{2}\right)T, \sigma^2 T\right]
Expected stock price:
E[ST]=S0⋅eμTE[S_T] = S_0 \cdot e^{\mu T}
Expected continuously compounded return (log return):
E[ln(STS0)]=(μ−σ22)TE\left[\ln\left(\frac{S_T}{S_0}\right)\right] = \left(\mu - \frac{\sigma^2}{2}\right)T
Note: Expected log return ≠\neq log of expected return.
Fractional Brownian Motion
Fractional Brownian motion (fBm) generalizes standard Brownian motion by allowing for correlation between increments. The Hurst exponent HH characterizes the process:
- H=0.5H = 0.5: Standard Brownian motion (independent increments)
- H>0.5H > 0.5: Positive correlation between increments (persistent/trending)
- H<0.5H < 0.5: Negative correlation (mean-reverting)
fBm with H<0.5H < 0.5 has been found useful for modeling volatility (rough volatility models).