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 ∫ 0 t f d u r α \int_0^t f\,du^{\alpha}_r ∫ 0 t f d u r α and of the observation integral ∫ 0 t f d u r \int_0^t f\,du_r ∫ 0 t f d u 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 X r α = X r + c r X^{\alpha}_r=X_r+c_r X r α = X r + c r almost surely for each r r r , so the integrand families ( ( f ( r ) E ~ ( r ) X r α ) i ) r \bigl((f(r)\tilde E(r)X^{\alpha}_r)^{i}\bigr)_r ( ( f ( r ) E ~ ( r ) X r α ) i ) r and ( ( f ( r ) E ~ ( r ) X r ) i + ( f ( r ) E ~ ( r ) c r ) i ) r \bigl((f(r)\tilde E(r)X_r)^{i}+(f(r)\tilde E(r)c_r)^{i}\bigr)_r ( ( f ( r ) E ~ ( r ) X r ) i + ( f ( r ) E ~ ( r ) c r ) i ) r are almost surely equal at each time; by the rule above and linearity, componentwise and almost surely,
∫ 0 t ( f ( r ) E ~ ( r ) X r α ) i d r = ∫ 0 t ( f ( r ) E ~ ( r ) X r ) i d r + ∫ 0 t ( f ( r ) E ~ ( r ) c r ) i d r , \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 , ∫ 0 t ( f ( r ) E ~ ( r ) X r α ) i d r = ∫ 0 t ( f ( r ) E ~ ( r ) X r ) i d r + ∫ 0 t ( f ( r ) E ~ ( r ) c r ) i d r ,
which is claim 1 (for t = 0 t=0 t = 0 all terms vanish by convention).
Claim 2. By claim 4 of Superposition Decomposition of the Controlled State and Observations , u x p α , j − u x p − 1 α , j = ( u x p j − u x p − 1 j ) + ( γ x p j − γ x p − 1 j ) 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) u x p α , j − u x p − 1 α , j = ( u x p j − u x p − 1 j ) + ( γ x p j − γ x p − 1 j ) 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 u u u converge componentwise in mean square to ∫ 0 t f d u r \int_0^t f\,du_r ∫ 0 t f d u r . By claim 1 above, it remains to show that, componentwise,
S n : = ∑ p = 1 n f ( x p − 1 ) ( γ x p − γ x p − 1 ) ⟶ ∫ 0 t f ( r ) ( E ~ ( r ) c r ) d r in 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.} S n := p = 1 ∑ n f ( x p − 1 ) ( γ x p − γ x p − 1 ) ⟶ ∫ 0 t f ( r ) ( E ~ ( r ) c r ) d r in mean square.
By claim 5 of Basic Properties of the Mean-Square Riemann Integral , γ x p j − γ x p − 1 j = ∫ x p − 1 x p ( E ~ ( r ) c r ) j d r \gamma^{j}_{x_p}-\gamma^{j}_{x_{p-1}}=\int_{x_{p-1}}^{x_p}(\tilde E(r)c_r)^{j}\,dr γ x p j − γ x p − 1 j = ∫ x p − 1 x p ( E ~ ( r ) c r ) j d r almost surely, and the target integral is the sum over p p p of ∫ x p − 1 x p ( f ( r ) E ~ ( r ) c r ) i d r \int_{x_{p-1}}^{x_p}\bigl(f(r)\tilde E(r)c_r\bigr)^{i}\,dr ∫ x p − 1 x p ( f ( r ) E ~ ( r ) c r ) i d r . Hence, componentwise and almost surely,
S n i − ( ∫ 0 t f ( r ) ( E ~ ( r ) c r ) d r ) i = ∑ p = 1 n ∫ x p − 1 x p ∑ j = 1 l ~ ( f ( x p − 1 ) − f ( r ) ) i j ( E ~ ( r ) c r ) j d r . 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 . S n i − ( ∫ 0 t f ( r ) ( E ~ ( r ) c r ) d r ) i = p = 1 ∑ n ∫ x p − 1 x p j = 1 ∑ l ~ ( f ( x p − 1 ) − f ( r ) ) ij ( E ~ ( r ) c r ) j d r .
Let ∥ ⋅ ∥ 2 \lVert\cdot\rVert_2 ∥ ⋅ ∥ 2 be the mean-square norm. Each function r ↦ ∥ ( E ~ ( r ) c r ) j ∥ 2 r\mapsto\lVert(\tilde E(r)c_r)^{j}\rVert_{2} r ↦ ∥( E ~ ( r ) c r ) j ∥ 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] [ 0 , t ] by some real C j C_j C j (Extreme Value Theorem on a Compact Interval ); put C : = max 1 ≤ j ≤ l ~ C j C:=\max_{1\le j\le\tilde l}C_j C := max 1 ≤ j ≤ l ~ C j . The entries of f f f are uniformly continuous on [ 0 , t ] [0,t] [ 0 , t ] by Continuity on a Closed Interval Implies Uniform Continuity ; write ω n \omega_n ω n for the maximum over entries ( i , j ) (i,j) ( i , j ) of the oscillation of f i j f_{ij} f ij over subintervals of length t / n t/n t / n , so ω n → 0 \omega_n\to0 ω n → 0 . By the triangle inequality and claims 4 and 6 of Basic Properties of the Mean-Square Riemann Integral ,
∥ S n i − ( ∫ 0 t f ( r ) ( E ~ ( r ) c r ) d r ) i ∥ 2 ≤ ∑ p = 1 n ∫ x p − 1 x p ∑ j = 1 l ~ ω n C d r = l ~ C t ω n ⟶ 0 , \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 , S n i − ( ∫ 0 t f ( r ) ( E ~ ( r ) c r ) d r ) i 2 ≤ p = 1 ∑ n ∫ x p − 1 x p j = 1 ∑ l ~ ω n C d r = l ~ C t ω n ⟶ 0 ,
which proves claim 2.
Claim 3. By claim 2 of The Kalman-Bucy Filter Equation and Its Solution , componentwise and almost surely,
m t f = E [ ξ ] + ∫ 0 t ( A ( r ) − K ( r ) E ~ ( r ) ) m r f d r + ∫ 0 t K ( r ) d u r ( 0 ≤ t ≤ T ) , 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), m t f = E [ ξ ] + ∫ 0 t ( A ( r ) − K ( r ) E ~ ( r ) ) m r f d r + ∫ 0 t K ( r ) d u r ( 0 ≤ t ≤ T ) ,
and by claim 1 of Superposition Decomposition of the Controlled State and Observations , c t = ∫ 0 t ( A ( r ) c r + B ( r ) α r ) d r c_t=\int_0^t\bigl(A(r)c_r+B(r)\alpha_r\bigr)\,dr c t = ∫ 0 t ( A ( r ) c r + B ( r ) α r ) d r almost surely. On the other hand, by claim 1 above with f = K f=K f = K ,
∫ 0 t K ( r ) d u r α = ∫ 0 t K ( r ) d u r + ∫ 0 t K ( r ) ( E ~ ( r ) c r ) d r almost 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.} ∫ 0 t K ( r ) d u r α = ∫ 0 t K ( r ) d u r + ∫ 0 t K ( r ) ( E ~ ( r ) c r ) d r 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 ] + ∫ 0 t ( ( A − K E ~ ) ( r ) X ^ r + B ( r ) α r ) d r + ∫ 0 t K ( r ) d u r α = E [ ξ ] + ∫ 0 t ( ( A − K E ~ ) ( r ) m r f ) d r + ∫ 0 t K ( r ) d u r + ∫ 0 t ( A ( r ) c r + B ( r ) α r ) d r , \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 , E [ ξ ] + ∫ 0 t ( ( A − K E ~ ) ( r ) X r + B ( r ) α r ) d r + ∫ 0 t K ( r ) d u r α = E [ ξ ] + ∫ 0 t ( ( A − K E ~ ) ( r ) m r f ) d r + ∫ 0 t K ( r ) d u r + ∫ 0 t ( A ( r ) c r + B ( r ) α r ) d r ,
since ( A − K E ~ ) ( m f + c ) + B α + K E ~ c = ( A − K E ~ ) m f + A c + B α (A-K\tilde E)(m^{\mathrm f}+c)+B\alpha+K\tilde Ec=(A-K\tilde E)m^{\mathrm f}+Ac+B\alpha ( A − K E ~ ) ( m f + c ) + B α + K E ~ c = ( A − K E ~ ) m f + A c + B α pointwise (componentwise algebra of the matrix-vector product ). By the two displayed equations for m f m^{\mathrm f} m f and c c c , the right-hand side equals m t f + c t = X ^ t m^{\mathrm f}_t+c_t=\widehat X_t m t f + c t = X t , which is the controlled filter equation.
For the equivalence: unpacking the definition of ∫ 0 t K d u r α \int_0^t K\,du^{\alpha}_r ∫ 0 t K d u r α 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 ] + ∫ 0 t ( ( A − K E ~ ) ( r ) X ^ r + K ( r ) E ~ ( r ) X r α + B ( r ) α r ) d r + ∑ j ′ = 1 m ∫ 0 t ( K ε ~ ) ⋅ j ′ ( r ) d W r j ′ , \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 , X t = E [ ξ ] + ∫ 0 t ( ( A − K E ~ ) ( r ) X r + K ( r ) E ~ ( r ) X r α + B ( r ) α r ) d r + j ′ = 1 ∑ m ∫ 0 t ( K ε ~ ) ⋅ j ′ ( r ) d W r j ′ ,
which, together with the mean-square continuity of the components of X ^ \widehat X 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 X is a mean-square solution of the linear stochastic differential equation with coefficient A − K E ~ A-K\tilde E A − K E ~ , forcing ( K ( r ) E ~ ( r ) X r α + B ( r ) α r ) r \bigl(K(r)\tilde E(r)X^{\alpha}_r+B(r)\alpha_r\bigr)_r ( K ( r ) E ~ ( r ) X r α + B ( r ) α r ) r , noise matrix K ε ~ K\tilde\varepsilon K ε ~ , and constant initial value E [ ξ ] \mathbb{E}[\xi] E [ ξ ] (the initial tuple is a constant, hence square-integrable, and the entries of K ε ~ K\tilde\varepsilon K ε ~ 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 □