TheoremBase

Brownian Increments After a Time are Independent of the Model Past

Statement

Throughout, a real-valued function on a subinterval II of the real numbers R\mathbb{R} is called continuous on II when it is continuous relative to II, both II and the codomain R\mathbb{R} carrying the metric of the real line. Consider a linear-Gaussian state-observation model on [0,T][0,T], with notation and fixed versions as there. Fix s∈[0,T]s\in[0,T] and let Hs\mathcal{H}_s denote the σ\sigma-algebra generated by the combined family of the random variables ξi\xi^{i} (1≤i≤l1\le i\le l), WrjW^{j}_r (1≤j≤m1\le j\le m, 0≤r≤s0\le r\le s), and urju^{j}_r (1≤j≤l~1\le j\le\tilde l, 0≤r≤s0\le r\le s). Since the values of uu up to time ss are Hs\mathcal{H}_s-measurable, Gs⊆Hs\mathcal{G}_s\subseteq\mathcal{H}_s.

1. (Independence of later increments) For every n≥1n\ge1 and all choices of component indices j1,…,jn∈{1,…,m}j_1,\dots,j_n\in\{1,\dots,m\} and times s≤up<vp≤Ts\le u_p<v_p\le T (1≤p≤n1\le p\le n), the σ\sigma-algebras

σ(Wv1j1−Wu1j1, …, Wvnjn−Wunjn)andHs\sigma\bigl(W^{j_1}_{v_1}-W^{j_1}_{u_1},\ \dots,\ W^{j_n}_{v_n}-W^{j_n}_{u_n}\bigr)\quad\text{and}\quad\mathcal{H}_s

are independent.

2. (Span structure of Wiener-integral increments) Let j∈{1,…,m}j\in\{1,\dots,m\}, let 0≤s<t≤T0\le s<t\le T, let f:[0,t]→Rf:[0,t]\to\mathbb{R} be continuous, and set

I:=∫0tf(r) dWrj−∫0sf(r) dWrj,I:=\int_0^t f(r)\,dW^{j}_r-\int_0^s f(r)\,dW^{j}_r ,

with Wiener integrals (any fixed versions; for s=0s=0 the subtracted term is 00 by the convention of Ito Integrable Process and the Ito Integral). Then E[I]=0\mathbb{E}[I]=0 with the expectation, and II lies in the closed mean-square span of the family of increments Wvj−WujW^{j}_v-W^{j}_u with s≤u<v≤ts\le u<v\le t.

3. (Orthogonality) With II as in claim 2, for every square-integrable random variable QQ that is almost surely equal to an Hs\mathcal{H}_s-measurable random variable: IQIQ is integrable, E[IQ]=0\mathbb{E}[IQ]=0, and, with the covariance, Cov⁡(I,Q)=0\operatorname{Cov}(I,Q)=0.

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