Let’s assume we have a probability space(Ω,F,P) and a martingale{(Xn,Fn)}. For a given stopping timeτ, Fτ:={A∈F:A∩(τ=n)∈Fn} is referred to as the sigma field induced by τ.
[1]: Fτ is a sigma field.
[2]: τ is a Fτ-measurable function.
[3]: For a martingale{(Xn,Fn)}, Xτ is a Fτ-measurable function.
[4]: 1(σ=n) is a Fσ-measurable function.
[5]: If Zn is a Fn-measurable function, then Zn1σ=n is both a Fσ-measurable function and a Fn-measurable function. Moreover, Zn1(σ=n)=Zσ1(σ=n) holds.
[6]: E(Xτ∣Fσ)1(σ=n)=E(Xτ∣Fn)1(σ=n) a.s.
Concerning Borel setsB∈B(R), with (τ∈B)=τ−1(B), (τ=n) is equivalent to τ−1({n}).
Given a stochastic process{Xn}n∈N0, regarding ω∈Ω, Xτ signifies the following:
Xτ=Xτ(ω)=Xτ(ω)(ω)
Explanation
A stopping time can essentially be understood as a random variable that represents a timing we are interested in.
Proof
[1]
To check if Fτ satisfies the conditions of a sigma field, we proceed as follows:
Part (i). ∅∈Fτ
Since F and Fn are sigma fields, they include ∅. Therefore, ∅∈Fτ holds.
Part (ii). A∈Fτ⟹Ac∈Fτ
Ac∩(τ=n)=(τ=n)∖[A∩(τ=n)]
where (τ=n)∈Fn, and if A∈Fτ, then by the definition of Fτ, A∩(τ=n)∈Fn follows, thus Ac∈Fτ
Part (iii). {An}n=1∞⊂Fτ⟹i=1⋃∞Ai∈Fτ
For i=1,2,⋯, if Ai∈Fτ then by the definition of Fτ, Ai∩(τ=n)∈Fn follows. Thus,
i=1⋃∞Ai∩(τ=n)=i=1⋃∞[Ai∩(τ=n)]∈Fn
Once again, by the definition of Fτ,
i=1⋃∞Ai∈Fτ
■
[2]
According to the equivalent conditions of a measurable function, to verify if τ is a Fτ-measurable function, it’s enough to check that for all k∈R, (τ≤k)∈Fτ holds.
(τ≤k)∩(τ=n)={∅(τ=n),k<n,k≥n
Here, ∅∈Fn and (τ=n)∈Fn, so regardless of what k∈R is, (τ≤k)∩(τ=n)∈Fn holds. Therefore, for all k∈R, (τ≤k)∈Fτ holds, and τ is a Fτ-measurable function.
■
[3]
For any Borel setB∈B(R), the following holds:
(Xτ∈B)∩(τ=n)=(Xn∈B)∩(τ=n)
This is because the reason (Xτ∈B) and (Xn∈B) are considered only when taking the intersection with (τ=n) results in only τ=n. It’s similar to how we only consider fixed cases when computing conditional expectationsE(Y∣X) as in X=x. Meanwhile, according to the definition of a martingale, (Xn∈B)∈Fn must hold, and by the definition of stopping time, (τ=n)∈Fn holds. Therefore, [(Xτ∈B)∩(τ=n)]∈Fτ, and Xτ is a Fτ-measurable function.
■
[4]
For event A∈F, 1A is represented as one of three possibilities:
(1A≤a)=⎩⎨⎧ΩAc∅,a≥1,a∈[0,1),a<0
Thus, given event A=(σ=n), for all Borel setsB∈B(R), ∅,(σ=n),Ω∈Fσ holds, so (1(σ=n)≤a)∈Fσ. In other words, 1(σ=n) is a Fσ-measurable function.
■
[5]
Zn1(σ=n)={Zσ⋅10,σ=n,σ=0
thus Zn1(σ=n)=Zσ1(σ=n) holds. [3] implicates that Zσ is a Fσ-measurable function, and [4] implies that 1(σ=n) is also a Fσ-measurable function, so their product, Zn1(σ=n), is also a Fσ-measurable function.
■
[6]
Since E(Xτ∣Fn) is Fn-measurable, E(Xτ∣Fn)1σ=n is Fσ-measurable by [4]. Meanwhile, 1(σ=n), due to the smoothing property, is a Fσ-measurable function, thus moving in and out of E(⋅∣Fσ) is permissible.
Furthermore, according to the properties above, for all A∈Fσ,
∫AE(Xτ∣Fσ)1(σ=n)dP======∫AE(Xτ1(σ=n)∣Fσ)dP∫AXτ1(σ=n)dP∫A∩(σ=n)XτdP∫AXτ1(σ=n)dP∫A∩(σ=n)E(Xτ∣Fn)dP∫AE(Xτ∣Fn)1(σ=n)dP∀A∈F,∫Afdm=0⟺f=0 a.e. hence,
E(Xτ∣Fσ)1(σ=n)=E(Xτ∣Fn)1(σ=n) a.s.