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Proof of Gaussian Structure and Moment Equations for Linear Stochastic Differential Equations

lemmalem:linear-sde-gaussian-covariance-2026a
Edited byClaude-agent-v2Aaron ·
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Reason: Reference update only: the citations of lem:second-moment-evolution-2026a are redirected to its corrected successor lem:second-moment-evolution-2026b (which adds the hypothesis 0 <= a < b; this proof only ever applies the lemma on [0,T], so nothing else changes). Part of the flag remediation requested by Aaron on 2026-07-31.

Proof

Claim 1. Write B\mathcal{B} for the base family of all ξi\xi^{i} and all WtjW^{j}_t, jointly Gaussian by hypothesis. Every member of the enlarged family is a mean-square limit of finite linear — hence affine — combinations of members of B\mathcal{B}: for the Wiener integrals this holds by claim 1 of Adapted Mean-Square Continuous Processes are Ito Integrable together with claim 1 of Existence and Uniqueness of the Mean-Square Extension of the Elementary Stochastic Integral (the elementary stochastic integrals of the deterministic grid-value approximants are finite linear combinations of increments of the WjW^{j}), and for the XtiX^{i}_t it is claim 3 of Existence, Uniqueness, and Variation of Constants for Linear Stochastic Differential Equations (with the forcing values absent, since every grg_r is the zero tuple). By Mean-Square Limits of Affine Combinations Adjoin to a Jointly Gaussian Family, the enlarged family is jointly Gaussian.

Claim 2. Taking expectations in the defining equation of Mean-Square Solution of a Linear Stochastic Differential Equation with Additive Wiener Noise (with vanishing forcing): Wiener integrals are centered (claim 2 of Wiener Integrals Against a Vector Brownian Motion are Jointly Gaussian), and by claim 3 of Basic Properties of the Mean-Square Riemann Integral (with Z=1Z=1) together with linearity of the expectation and of the Riemann integral (Agreement of the Riemann and Lebesgue Integrals for Continuous Functions on a Closed Interval, Linearity and Monotonicity of the Lebesgue Integral),

μi(t)=E[ξi]+0tjAij(r)μj(r)dr(0tT),\mu^{i}(t)=\mathbb{E}[\xi^{i}]+\int_0^t\sum_jA_{ij}(r)\,\mu^{j}(r)\,dr\qquad(0\le t\le T),

with μi\mu^{i} continuous (claim 3 of Basic Properties of the Mean-Square Riemann Integral). This is the linear system of claim 3 of Fundamental Solution and Variation of Constants for Linear Ordinary Differential Equations with vanishing inhomogeneity on [0,T][0,T], whose unique continuous solution is Φ(t)E[ξ]\Phi(t)\,\mathbb{E}[\xi].

Claim 3. Fix i,ki,k. The pair (Y,Z)=(Xi,Xk)(Y,Z)=(X^{i},X^{k}) is of the form treated in Second-Moment Evolution for Processes of Integral Form on [0,T][0,T]: Xti=ξi+0tαrdr+j0tεij(r)dWrjX^{i}_t=\xi^{i}+\int_0^t\alpha_r\,dr+\sum_j\int_0^t\varepsilon_{ij}(r)\,dW^{j}_r with αr=jAij(r)Xrj\alpha_r=\sum_jA_{ij}(r)X^{j}_r, mean-square continuous by claims 1-2 of Basic Properties of the Mean-Square Riemann Integral (and similarly for XkX^{k}). The orthogonality hypothesis of that lemma holds by its claim 2: for every ss, XsiX^{i}_s and XskX^{k}_s lie in the closed mean-square span of the ξi\xi^{i'} and the WrjW^{j'}_r with rsr\le s (claim 3 of Existence, Uniqueness, and Variation of Constants for Linear Stochastic Differential Equations), and σ(ξ1,,ξl)\sigma(\xi^{1},\dots,\xi^{l}) is independent of the WW-σ\sigma-algebra by hypothesis. Hence, by claim 1 of Second-Moment Evolution for Processes of Integral Form,

E[XtiXtk]=E[ξiξk]+0t(jAijE[XrjXrk]+jAkjE[XriXrj]+jεijεkj(r))dr.\mathbb{E}[X^{i}_tX^{k}_t]=\mathbb{E}[\xi^{i}\xi^{k}]+\int_0^t\Bigl(\sum_jA_{ij}\,\mathbb{E}[X^{j}_rX^{k}_r]+\sum_jA_{kj}\,\mathbb{E}[X^{i}_rX^{j}_r]+\sum_j\varepsilon_{ij}\varepsilon_{kj}(r)\Bigr)dr .

The functions μi\mu^{i} are continuous and, by Fundamental Theorem of Calculus, Part I in One Dimension applied to claim 2's integral equation, differentiable at interior points with (μi)=jAijμj(\mu^{i})'=\sum_jA_{ij}\mu^{j}; the product rule (Sum and Product Rules for One-Dimensional Derivatives and Continuity) gives that μiμk\mu^{i}\mu^{k} is continuous on [0,T][0,T], differentiable at interior points with derivative jAijμjμk+μijAkjμj\sum_jA_{ij}\mu^{j}\mu^{k}+\mu^{i}\sum_jA_{kj}\mu^{j}, hence an antiderivative of that continuous function, and Fundamental Theorem of Calculus, Part II in One Dimension gives the corresponding integral identity. Subtracting it from the display above and using Cov(Xti,Xtk)=E[XtiXtk]μi(t)μk(t)\operatorname{Cov}(X^{i}_t,X^{k}_t)=\mathbb{E}[X^{i}_tX^{k}_t]-\mu^{i}(t)\mu^{k}(t) (Covariance of Square-Integrable Random Variables) and linearity of the Riemann integral,

Pik(t)=Pik(0)+0t(jAij(r)Pjk(r)+jAkj(r)Pij(r)+(εε)ik(r))dr,P_{ik}(t)=P_{ik}(0)+\int_0^t\Bigl(\sum_jA_{ij}(r)P_{jk}(r)+\sum_jA_{kj}(r)P_{ij}(r)+(\varepsilon\varepsilon^{\top})_{ik}(r)\Bigr)dr ,

with Pik(0)=E[ξiξk]E[ξi]E[ξk]=Cov(ξi,ξk)P_{ik}(0)=\mathbb{E}[\xi^{i}\xi^{k}]-\mathbb{E}[\xi^{i}]\mathbb{E}[\xi^{k}]=\operatorname{Cov}(\xi^{i},\xi^{k}). Since Pij=PjiP_{ij}=P_{ji} (symmetry of the covariance), jAkjPij=(PA)ik\sum_jA_{kj}P_{ij}=(PA^{\top})_{ik} by Product of Real Matrices and Transpose of a Real Matrix, and jεijεkj=(εε)ik\sum_j\varepsilon_{ij}\varepsilon_{kj}=(\varepsilon\varepsilon^{\top})_{ik}, this is exactly the asserted entrywise equation. Its entries are continuous (claim 1 of Second-Moment Evolution for Processes of Integral Form and continuity of μiμk\mu^{i}\mu^{k}), so PP is a continuous solution of the equation of claim 1 of Lyapunov Representation and Positive Semidefiniteness for Linear Matrix Equations for the data (A,εε,P0)(A,\varepsilon\varepsilon^{\top},P_0), hence the unique one. \blacksquare

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