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Proof of Integrals Against the Controlled Observations and the Controlled Filter Equation

lemmalem:controlled-observation-integrals-2026a
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Reason: Proof of lem:controlled-observation-integrals-2026a (separation-theorem block D2). Internally reviewed and validated; approved by Aaron on 2026-07-31.

Proof

Throughout, we use the rule (as in the proof of Superposition Decomposition of the Controlled State and Observations) that mean-square continuous integrand families that are almost surely equal at each time have almost surely equal mean-square Riemann integrals, and linearity and additivity of those integrals (claims 1 and 5 of Basic Properties of the Mean-Square Riemann Integral).

Claim 1. The Wiener-integral parts of 0tfdurα\int_0^t f\,du^{\alpha}_r and of the observation integral 0tfdur\int_0^t f\,du_r of Integrals Against the Observation Process are Determined by the Observations are the same fixed versions. For the mean-square Riemann parts, claim 2 of Superposition Decomposition of the Controlled State and Observations gives Xrα=Xr+crX^{\alpha}_r=X_r+c_r almost surely for each rr, so the integrand families ((f(r)E~(r)Xrα)i)r\bigl((f(r)\tilde E(r)X^{\alpha}_r)^{i}\bigr)_r and ((f(r)E~(r)Xr)i+(f(r)E~(r)cr)i)r\bigl((f(r)\tilde E(r)X_r)^{i}+(f(r)\tilde E(r)c_r)^{i}\bigr)_r are almost surely equal at each time; by the rule above and linearity, componentwise and almost surely,

0t(f(r)E~(r)Xrα)idr=0t(f(r)E~(r)Xr)idr+0t(f(r)E~(r)cr)idr,\int_0^t\bigl(f(r)\tilde E(r)X^{\alpha}_r\bigr)^{i}\,dr=\int_0^t\bigl(f(r)\tilde E(r)X_r\bigr)^{i}\,dr+\int_0^t\bigl(f(r)\tilde E(r)c_r\bigr)^{i}\,dr ,

which is claim 1 (for t=0t=0 all terms vanish by convention).

Claim 2. By claim 4 of Superposition Decomposition of the Controlled State and Observations, uxpα,juxp1α,j=(uxpjuxp1j)+(γxpjγxp1j)u^{\alpha,j}_{x_p}-u^{\alpha,j}_{x_{p-1}}=\bigl(u^{j}_{x_p}-u^{j}_{x_{p-1}}\bigr)+\bigl(\gamma^{j}_{x_p}-\gamma^{j}_{x_{p-1}}\bigr) almost surely, so the Riemann-Stieltjes sums split accordingly. By claim 1 of Integrals Against the Observation Process are Determined by the Observations, the sums formed with uu converge componentwise in mean square to 0tfdur\int_0^t f\,du_r. By claim 1 above, it remains to show that, componentwise,

Sn:=p=1nf(xp1)(γxpγxp1)  0tf(r)(E~(r)cr)drin mean square.S_n:=\sum_{p=1}^{n}f(x_{p-1})\bigl(\gamma_{x_p}-\gamma_{x_{p-1}}\bigr)\ \longrightarrow\ \int_0^t f(r)\bigl(\tilde E(r)c_r\bigr)\,dr\qquad\text{in mean square.}

By claim 5 of Basic Properties of the Mean-Square Riemann Integral, γxpjγxp1j=xp1xp(E~(r)cr)jdr\gamma^{j}_{x_p}-\gamma^{j}_{x_{p-1}}=\int_{x_{p-1}}^{x_p}(\tilde E(r)c_r)^{j}\,dr almost surely, and the target integral is the sum over pp of xp1xp(f(r)E~(r)cr)idr\int_{x_{p-1}}^{x_p}\bigl(f(r)\tilde E(r)c_r\bigr)^{i}\,dr. Hence, componentwise and almost surely,

Sni(0tf(r)(E~(r)cr)dr)i=p=1nxp1xpj=1l~(f(xp1)f(r))ij(E~(r)cr)jdr.S^{i}_n-\Bigl(\int_0^t f(r)\bigl(\tilde E(r)c_r\bigr)\,dr\Bigr)^{i}=\sum_{p=1}^{n}\int_{x_{p-1}}^{x_p}\sum_{j=1}^{\tilde l}\bigl(f(x_{p-1})-f(r)\bigr)_{ij}\bigl(\tilde E(r)c_r\bigr)^{j}\,dr .

Let 2\lVert\cdot\rVert_2 be the mean-square norm. Each function r(E~(r)cr)j2r\mapsto\lVert(\tilde E(r)c_r)^{j}\rVert_{2} is continuous (claim 4 of Basic Properties of the Mean-Square Riemann Integral, the integrand family being mean-square continuous by claims 1-2 there), hence bounded on [0,t][0,t] by some real CjC_j (Extreme Value Theorem on a Compact Interval); put C:=max1jl~CjC:=\max_{1\le j\le\tilde l}C_j. The entries of ff are uniformly continuous on [0,t][0,t] by Continuity on a Closed Interval Implies Uniform Continuity; write ωn\omega_n for the maximum over entries (i,j)(i,j) of the oscillation of fijf_{ij} over subintervals of length t/nt/n, so ωn0\omega_n\to0. By the triangle inequality and claims 4 and 6 of Basic Properties of the Mean-Square Riemann Integral,

Sni(0tf(r)(E~(r)cr)dr)i2p=1nxp1xpj=1l~ωnCdr=l~Ctωn0,\Bigl\lVert S^{i}_n-\Bigl(\int_0^t f(r)\bigl(\tilde E(r)c_r\bigr)\,dr\Bigr)^{i}\Bigr\rVert_{2}\le\sum_{p=1}^{n}\int_{x_{p-1}}^{x_p}\sum_{j=1}^{\tilde l}\omega_n\,C\,dr=\tilde l\,C\,t\,\omega_n\longrightarrow0 ,

which proves claim 2.

Claim 3. By claim 2 of The Kalman-Bucy Filter Equation and Its Solution, componentwise and almost surely,

mtf=E[ξ]+0t(A(r)K(r)E~(r))mrfdr+0tK(r)dur(0tT),m^{\mathrm f}_t=\mathbb{E}[\xi]+\int_0^t\bigl(A(r)-K(r)\tilde E(r)\bigr)m^{\mathrm f}_r\,dr+\int_0^t K(r)\,du_r\qquad(0\le t\le T),

and by claim 1 of Superposition Decomposition of the Controlled State and Observations, ct=0t(A(r)cr+B(r)αr)drc_t=\int_0^t\bigl(A(r)c_r+B(r)\alpha_r\bigr)\,dr almost surely. On the other hand, by claim 1 above with f=Kf=K,

0tK(r)durα=0tK(r)dur+0tK(r)(E~(r)cr)dralmost surely.\int_0^t K(r)\,du^{\alpha}_r=\int_0^t K(r)\,du_r+\int_0^t K(r)\bigl(\tilde E(r)c_r\bigr)\,dr\qquad\text{almost surely.}

Therefore, using linearity and the rule for almost surely equal integrands (all integrand families being mean-square continuous), componentwise and almost surely,

E[ξ]+0t((AKE~)(r)X^r+B(r)αr)dr+0tK(r)durα=E[ξ]+0t((AKE~)(r)mrf)dr+0tK(r)dur+0t(A(r)cr+B(r)αr)dr,\mathbb{E}[\xi]+\int_0^t\Bigl(\bigl(A-K\tilde E\bigr)(r)\widehat X_r+B(r)\alpha_r\Bigr)dr+\int_0^t K(r)\,du^{\alpha}_r=\mathbb{E}[\xi]+\int_0^t\Bigl(\bigl(A-K\tilde E\bigr)(r)m^{\mathrm f}_r\Bigr)dr+\int_0^t K(r)\,du_r+\int_0^t\bigl(A(r)c_r+B(r)\alpha_r\bigr)dr ,

since (AKE~)(mf+c)+Bα+KE~c=(AKE~)mf+Ac+Bα(A-K\tilde E)(m^{\mathrm f}+c)+B\alpha+K\tilde Ec=(A-K\tilde E)m^{\mathrm f}+Ac+B\alpha pointwise (componentwise algebra of the matrix-vector product). By the two displayed equations for mfm^{\mathrm f} and cc, the right-hand side equals mtf+ct=X^tm^{\mathrm f}_t+c_t=\widehat X_t, which is the controlled filter equation.

For the equivalence: unpacking the definition of 0tKdurα\int_0^t K\,du^{\alpha}_r and combining the two mean-square Riemann integrals by linearity, the controlled filter equation states exactly that, componentwise and almost surely,

X^t=E[ξ]+0t((AKE~)(r)X^r+K(r)E~(r)Xrα+B(r)αr)dr+j=1m0t(Kε~)j(r)dWrj,\widehat X_t=\mathbb{E}[\xi]+\int_0^t\Bigl(\bigl(A-K\tilde E\bigr)(r)\widehat X_r+K(r)\tilde E(r)X^{\alpha}_r+B(r)\alpha_r\Bigr)dr+\sum_{j'=1}^{m}\int_0^t\bigl(K\tilde\varepsilon\bigr)_{\cdot j'}(r)\,dW^{j'}_r ,

which, together with the mean-square continuity of the components of X^\widehat X (claim 1 of Conditional Expectation and Estimation Error of the Controlled State) and of the forcing family (claims 1-2 of Basic Properties of the Mean-Square Riemann Integral), says precisely that X^\widehat X is a mean-square solution of the linear stochastic differential equation with coefficient AKE~A-K\tilde E, forcing (K(r)E~(r)Xrα+B(r)αr)r\bigl(K(r)\tilde E(r)X^{\alpha}_r+B(r)\alpha_r\bigr)_r, noise matrix Kε~K\tilde\varepsilon, and constant initial value E[ξ]\mathbb{E}[\xi] (the initial tuple is a constant, hence square-integrable, and the entries of Kε~K\tilde\varepsilon are continuous). Uniqueness among componentwise mean-square continuous square-integrable families satisfying the displayed equation is claim 2 of Existence, Uniqueness, and Variation of Constants for Linear Stochastic Differential Equations applied to this equation. \square

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