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Proof of Brownian Increments After a Time are Independent of the Model Past

lemmalem:brownian-increments-independent-model-past-2026a
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Reason: Proof of lem:brownian-increments-independent-model-past-2026a (separation-theorem block D2). Internally reviewed and validated; approved by Aaron on 2026-07-31.

Proof

Throughout, 2\lVert\cdot\rVert_{2} is the mean-square norm of Square-Integrable Random Variables and the Mean-Square Inner Product, and the covariance is bilinear in each argument (by linearity of the integral, Linearity and Monotonicity of the Lebesgue Integral, applied to its defining formula) and satisfies, for square-integrable XX and YnYY_n\to Y in mean square, Cov(X,Yn)Cov(X,Y)\operatorname{Cov}(X,Y_n)\to\operatorname{Cov}(X,Y): indeed Cov(X,YnY)=E[X(YnY)]E[X]E[YnY]2X2YnY2|\operatorname{Cov}(X,Y_n-Y)|=|\mathbb{E}[X(Y_n-Y)]-\mathbb{E}[X]\mathbb{E}[Y_n-Y]|\le2\lVert X\rVert_{2}\lVert Y_n-Y\rVert_{2} by Cauchy-Schwarz and Triangle Inequalities for the Mean-Square Norm (the constant E[X]\mathbb{E}[X] having E[X]2X2\lVert\mathbb{E}[X]\rVert_2\le\lVert X\rVert_2).

Claim 1. Step 1: vanishing cross-covariances. Fix an increment D=WvjWujD=W^{j}_{v}-W^{j}_{u} with su<vTs\le u<v\le T. We check that DD is uncorrelated with every member of the generating family of Hs\mathcal{H}_s.

(a) For ξi\xi^{i}: σ(ξ1,,ξl)\sigma(\xi^{1},\dots,\xi^{l}) is independent of σ(Wrj:1jm, r0)\sigma(W^{j'}_r:1\le j'\le m,\ r\ge0) by the model, so ξi\xi^{i} is independent of WvjW^{j}_{v} and of WujW^{j}_{u}; by Expectation of a Product of Independent Random Variables and bilinearity, Cov(D,ξi)=Cov(Wvj,ξi)Cov(Wuj,ξi)=0\operatorname{Cov}(D,\xi^{i})=\operatorname{Cov}(W^{j}_v,\xi^{i})-\operatorname{Cov}(W^{j}_u,\xi^{i})=0.

(b) For WrjW^{j'}_r with 0rs0\le r\le s: by the covariances of claim 3 of Wiener Integrals Against a Vector Brownian Motion are Jointly Gaussian, if j=jj'=j then Cov(D,Wrj)=min(v,r)min(u,r)=rr=0\operatorname{Cov}(D,W^{j}_r)=\min(v,r)-\min(u,r)=r-r=0 since rsu<vr\le s\le u<v, and if jjj'\ne j both covariances vanish.

(c) For uqju^{j''}_q with 0qs0\le q\le s: by claim 1 of Gaussian and Span Structure of the Linear-Gaussian State-Observation Model, uqju^{j''}_q is a mean-square limit of finite linear combinations of the ξi\xi^{i} and the WrjW^{j'}_r with rqsr\le q\le s; by (a), (b), bilinearity, and the mean-square continuity of the covariance stated above, Cov(D,uqj)=0\operatorname{Cov}(D,u^{j''}_q)=0.

Step 2: independence from finite generator blocks. Fix increments D1,,DnD_1,\dots,D_n as in the claim and finitely many random variables g1,,gdg_1,\dots,g_d, each of which is one of the ξi\xi^{i}, one of the WrjW^{j'}_r (rsr\le s), or one of the uqju^{j''}_q (qsq\le s). By claim 2 of Gaussian and Span Structure of the Linear-Gaussian State-Observation Model, the combined family of all ξi\xi^{i}, WrjW^{j'}_r, XriX^{i}_r, and urju^{j''}_r is jointly Gaussian; hence the finite tuple (Wv1j1,Wu1j1,,Wvnjn,Wunjn,g1,,gd)(W^{j_1}_{v_1},W^{j_1}_{u_1},\dots,W^{j_n}_{v_n},W^{j_n}_{u_n},g_1,\dots,g_d) is a Gaussian random vector, and so is its linear image (D1,,Dn,g1,,gd)(D_1,\dots,D_n,g_1,\dots,g_d) by Affine Transformations of Gaussian Random Vectors are Gaussian. Every Cov(Dp,gd)\operatorname{Cov}(D_p,g_{d'}) vanishes by Step 1, so by Uncorrelated Jointly Gaussian Blocks are Independent the σ\sigma-algebras σ(D1,,Dn)\sigma(D_1,\dots,D_n) and σ(g1,,gd)\sigma(g_1,\dots,g_d) are independent.

Step 3: independence from Hs\mathcal{H}_s. Let P\mathcal{P} be the collection of all finite intersections of events of the form g1(B)g^{-1}(B), where gg ranges over the generating family of Hs\mathcal{H}_s and BB over Borel sets. Then P\mathcal{P} is a π\pi-system in the sense of Dynkin's Pi-Lambda Theorem: it is nonempty (Ω\Omega is the preimage of R\mathbb{R} under ξ1\xi^{1}) and closed under finite intersections by construction; and the generated σ\sigma-algebra σ(P)\sigma(\mathcal{P}) equals Hs\mathcal{H}_s, since each contains the other's generators. Let

L:={BF: P(AB)=P(A)P(B) for every Aσ(D1,,Dn)}.\mathcal{L}:=\{B\in\mathcal{F}:\ P(A\cap B)=P(A)P(B)\ \text{for every}\ A\in\sigma(D_1,\dots,D_n)\}.

Then L\mathcal{L} is a λ\lambda-system in the sense of Dynkin's Pi-Lambda Theorem: ΩL\Omega\in\mathcal{L}; if BBB\subseteq B' both lie in L\mathcal{L} then P(A(BB))=P(AB)P(AB)=P(A)(P(B)P(B))=P(A)P(BB)P(A\cap(B'\setminus B))=P(A\cap B')-P(A\cap B)=P(A)\bigl(P(B')-P(B)\bigr)=P(A)P(B'\setminus B); and for an increasing sequence BnBB_n\uparrow B in L\mathcal{L}, continuity of the measure from below gives P(AB)=limP(ABn)=P(A)limP(Bn)=P(A)P(B)P(A\cap B)=\lim P(A\cap B_n)=P(A)\lim P(B_n)=P(A)P(B). Every member of P\mathcal{P} lies in σ(g1,,gd)\sigma(g_1,\dots,g_d) for the finite family of generators appearing in it, so PL\mathcal{P}\subseteq\mathcal{L} by Step 2. By Dynkin's Pi-Lambda Theorem, Hs=σ(P)L\mathcal{H}_s=\sigma(\mathcal{P})\subseteq\mathcal{L}, which is exactly the asserted independence.

Claim 2. E[I]=0\mathbb{E}[I]=0 since Wiener integrals have expectation zero (claim 2 of Wiener Integrals Against a Vector Brownian Motion are Jointly Gaussian) and expectation is linear. For the span assertion, recall from Wiener Integrals Against a Vector Brownian Motion are Jointly Gaussian that 0tf(r)dWrj\int_0^{t}f(r)\,dW^{j}_r is the It^{o} integral of (f(r))r(0,t](f(r))_{r\in(0,t]} with respect to the It^{o} integrator (Wj,1)(W^{j},1) of Brownian Motion is an Ito Integrator with Unit Intensity, for the natural filtration of WjW^{j}, and that 0sf(r)dWrj\int_0^{s}f(r)\,dW^{j}_r is the It^{o} integral of the restriction of ff to (0,s](0,s], by the subinterval paragraph of Ito Integrable Process and the Ito Integral (for s=0s=0 it is 00 and the assertion reduces to the case treated below with no pieces to the left of ss).

For n1n\ge1, let 0=y0<y1<<yN(n)=t0=y_0<y_1<\dots<y_{N(n)}=t be the partition of [0,t][0,t] whose point set is {pt/n:0pn}{s}\{pt/n:0\le p\le n\}\cup\{s\} (listed strictly increasingly), and define the deterministic simple adapted process fnf_n on (0,t](0,t] by fn(r):=f(yp1)f_n(r):=f(y_{p-1}) for r(yp1,yp]r\in(y_{p-1},y_p]. Since ff is uniformly continuous on the compact interval [0,t][0,t] by Continuity on a Closed Interval Implies Uniform Continuity, and the mesh of these partitions tends to 00, we have ϵn:=supr(0,t]fn(r)f(r)0\epsilon_n:=\sup_{r\in(0,t]}|f_n(r)-f(r)|\to0. Hence (fn)(f_n) is an approximating sequence for (f(r))r(0,t](f(r))_{r\in(0,t]} in the sense of Existence and Uniqueness of the Mean-Square Extension of the Elementary Stochastic Integral: for its Cauchy-type condition (a), the intensity of the integrator (Wj,1)(W^{j},1) is the constant 11, and for all n,nn,n' the deterministic simple processes satisfy R1(0,t](r)E[(fn(r)fn(r))2]drt(ϵn+ϵn)20\int_{\mathbb{R}}\mathbf{1}_{(0,t]}(r)\,\mathbb{E}\bigl[(f_n(r)-f_{n'}(r))^{2}\bigr]\,dr\le t\,(\epsilon_n+\epsilon_{n'})^{2}\to0; and for its pointwise condition (b), at each r(0,t]r\in(0,t] we have fn(r)f(r)2=fn(r)f(r)ϵn0\lVert f_n(r)-f(r)\rVert_{2}=|f_n(r)-f(r)|\le\epsilon_n\to0. The restrictions of the fnf_n to (0,s](0,s] form an approximating sequence for the restriction of ff, by the subinterval paragraph of Ito Integrable Process and the Ito Integral. By claims 1-2 of Existence and Uniqueness of the Mean-Square Extension of the Elementary Stochastic Integral (claim 1 producing a limit of the elementary stochastic integrals, claim 2 identifying it, up to almost sure equality, with any version of the It^{o} integral), the elementary stochastic integrals of fnf_n over (0,t](0,t] and over (0,s](0,s] converge in mean square to 0tfdWj\int_0^t f\,dW^{j} and 0sfdWj\int_0^s f\,dW^{j} respectively. By Elementary Stochastic Integral of a Simple Adapted Process, the difference of the two elementary integrals is

In:=p:yp1sf(yp1)(WypjWyp1j),I_n:=\sum_{p:\,y_{p-1}\ge s}f(y_{p-1})\bigl(W^{j}_{y_p}-W^{j}_{y_{p-1}}\bigr),

a finite linear combination of increments WvjWujW^{j}_v-W^{j}_u with su<vts\le u<v\le t (the partition contains ss, so every subinterval lies entirely in [0,s][0,s] or in [s,t][s,t]). Then InI20\lVert I_n-I\rVert_2\to0, so II lies in the closed mean-square span of these increments.

Claim 3. Let Q~\tilde Q be an Hs\mathcal{H}_s-measurable random variable almost surely equal to QQ. With InI_n as in claim 2: each InI_n is measurable with respect to the σ\sigma-algebra generated by the finitely many increments appearing in it (preimages under a continuous, hence Borel, linear combination), which is independent of Hs\mathcal{H}_s by claim 1; hence InI_n and Q~\tilde Q are independent, and by Expectation of a Product of Independent Random Variables, E[InQ~]=E[In]E[Q~]=0\mathbb{E}[I_n\tilde Q]=\mathbb{E}[I_n]\,\mathbb{E}[\tilde Q]=0, each increment having expectation 00 (claim 2 of Wiener Integrals Against a Vector Brownian Motion are Jointly Gaussian and linearity of the expectation). By Cauchy-Schwarz and Triangle Inequalities for the Mean-Square Norm, E[IQ~]E[InQ~]IIn2Q~20|\mathbb{E}[I\tilde Q]-\mathbb{E}[I_n\tilde Q]|\le\lVert I-I_n\rVert_2\lVert\tilde Q\rVert_2\to0, so E[IQ~]=0\mathbb{E}[I\tilde Q]=0; the product IQ~I\tilde Q is integrable by Cauchy-Schwarz and Triangle Inequalities for the Mean-Square Norm. Since IQ=IQ~IQ=I\tilde Q almost surely, IQIQ is integrable with E[IQ]=0\mathbb{E}[IQ]=0, and Cov(I,Q)=E[IQ]E[I]E[Q]=0\operatorname{Cov}(I,Q)=\mathbb{E}[IQ]-\mathbb{E}[I]\mathbb{E}[Q]=0 by claim 2. \square

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