1. Without randomness
(Notation)
- X(t)= the position of the particle at time t.
- μ(t,x)= drift term = the velocity of the particle when it is located at x at time t.
- Δt= a very small change in time.
- ΔX(t)=X(t+Δt)−X(t)= a very small change in location from time t to time t+Δt
When a particle moves on the real line without randomness, its trajectory can be described by ΔX(t)=μ(t,X(t))Δt
We can determine X(t) by solving ordinary differential equation X˙(t).
X(t+Δt)=X(t)+μ(t,X(t))Δt
⇒ ΔtX(t+Δt)−X(t)=μ(t,X(t))
⇒ ΔtΔX(t)=μ(t,X(t))
⇒ X˙(t)=μ(t,X(t))
2. With randomness
(Notation)
- W(t)=Wt= the Wiener process.
- ΔW(t)=W(t+Δt)−W(t)= the displacement by the Brownian motion from time t to time t+Δt
- σ(t,x)= diffusion term measuring the strength of randomness.
With randomness, its trajectory can be described by ΔtΔX(t)=μ(t,X(t))+σ(t,X(t))ΔtΔW(t)
However we cannot solve X˙(t)=μ(t,X(t))+σ(t,X(t))W˙(t) because W(t) is not differentiable.
Instead, we can rewrite its trajectory
dX(t)=μ(t,X(t))dt+σ(t,X(t))dW(t)
Then, integrate both sides
∫otdX(s)=∫0tμ(s,X(s))ds+∫0tσ(s,X(s))dW(s)
⇒ X(t,w)=X0+∫0tμ(s,X(s,w))ds+∫0tσ(s,X(s,w))dW(s,w)
Let X be a stochastic process.
- FtX= σ-algebra generated by X on the time interval [0,t]. It is called the infromation generated by X on [0,t]
- If a random variable Z:Ω→R which is probabilities of events in term of Z can be calculated based on the σ-algebra FtX, then we write Z∈FtX. Z is said to be FtX-measurable
- If another stochastic process Y(t) satisfies Y(t)∈FtX for all t≥0, Y is said to be adapted to the filtration F={FtX}t≥0