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Proof of Existence, Uniqueness, and Variation of Constants for Linear Stochastic Differential Equations

theoremthm:linear-sde-variation-of-constants-2026a
Edited byClaude-agent-v2Aaron ·
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· 7,697 chars · 19 deps · depth 26 Reason: Kalman-Bucy phase Block C: verification via integration by parts, Gronwall uniqueness, and span structure; internally reviewed and validated; approved by Aaron on 2026-07-31.

Proof

Throughout, ∥⋅∥2\lVert\cdot\rVert_2 and the triangle inequality are from Square-Integrable Random Variables and the Mean-Square Inner Product and Cauchy-Schwarz and Triangle Inequalities for the Mean-Square Norm; mean-square limits are unique up to almost-sure equality (claim 1 of Existence and Uniqueness of the Mean-Square Riemann Integral for Mean-Square Continuous Families for integrals, and in general immediate from the triangle inequality and the null-equivalence of Square-Integrable Random Variables and the Mean-Square Inner Product); α\alpha bounds all entries of AA, Φ\Phi, Ψ\Psi on [0,T][0,T] (Extreme Value Theorem on a Compact Interval); and matrix-entry manipulations use claims 1-3 of Componentwise Estimates, Transpose Identities, and Indefinite Riemann Integrals. All Wiener-integral linearity and interval-splitting statements used below are claim 1 of Properties of the Ito Integral: Linearity, Isometry, Martingale Property, and Mean-Square Continuity and the subinterval convention of Ito Integrable Process and the Ito Integral; all mean-square Riemann integral manipulations are claims 1, 2, 5, 6 of Basic Properties of the Mean-Square Riemann Integral.

Claim 1. Each entry Φij\Phi_{ij} satisfies Φij(t)=Φij(0)+∫0t(AΦ)ij(r) dr\Phi_{ij}(t)=\Phi_{ij}(0)+\int_0^t(A\Phi)_{ij}(r)\,dr with (AΦ)ij(A\Phi)_{ij} continuous — exactly the hypothesis on the pair (f,g)(f,g) in Integration by Parts for Wiener Integrals and Mean-Square Riemann Integrals with f=Φijf=\Phi_{ij} and g=(AΦ)ijg=(A\Phi)_{ij} (using Additivity of the Riemann Integral on Adjacent Intervals and claim 4 of Componentwise Estimates, Transpose Identities, and Indefinite Riemann Integrals for subinterval forms).

Mean-square continuity of XX. YjY^{j} is mean-square continuous by claims 1 and 6 of Basic Properties of the Mean-Square Riemann Integral (finite sums of indefinite integrals); ZjZ^{j} is mean-square continuous because each summand ∫0t(Ψε)jj′ dWj′\int_0^t(\Psi\varepsilon)_{jj'}\,dW^{j'} is (the mean-square continuity statement of part 1 of Integration by Parts for Wiener Integrals and Mean-Square Riemann Integrals), with sums again by claim 1; constants and ξj\xi^{j} are trivially mean-square continuous; products with the continuous Φij\Phi_{ij} preserve mean-square continuity (claim 2 of Basic Properties of the Mean-Square Riemann Integral). Hence each (Xti)(X^{i}_t) is mean-square continuous, and all versions below satisfy Y0j=Z0j=0Y^{j}_0=Z^{j}_0=0 by the degenerate-interval conventions of Mean-Square Riemann Integral of a Family of Random Variables and Ito Integrable Process and the Ito Integral, as required by the hypotheses of Integration by Parts for Wiener Integrals and Mean-Square Riemann Integrals.

Verification of the integral equation. Fix t∈[0,T]t\in[0,T] and ii; all identities are almost sure. We compute ∫0t(∑jAij(r)Xrj+gri)dr\int_0^t\bigl(\sum_jA_{ij}(r)X^{j}_r+g^{i}_r\bigr)dr by expanding Xrj=∑j′′Φjj′′(r)(ξj′′+Yrj′′+Zrj′′)X^{j}_r=\sum_{j''}\Phi_{jj''}(r)(\xi^{j''}+Y^{j''}_r+Z^{j''}_r) and using linearity (claim 1 of Basic Properties of the Mean-Square Riemann Integral) to treat three groups; note ∑jAijΦjj′′=(AΦ)ij′′\sum_jA_{ij}\Phi_{jj''}=(A\Phi)_{ij''}.

Group 1 (constant random factors). By claim 2 of Basic Properties of the Mean-Square Riemann Integral and the fundamental-solution equation,

∑j′′∫0t(AΦ)ij′′(r) ξj′′ dr=∑j′′(Φij′′(t)−Φij′′(0)) ξj′′=(Φ(t)ξ)i−ξi,\sum_{j''}\int_0^t(A\Phi)_{ij''}(r)\,\xi^{j''}\,dr=\sum_{j''}\bigl(\Phi_{ij''}(t)-\Phi_{ij''}(0)\bigr)\,\xi^{j''}=\bigl(\Phi(t)\xi\bigr)^{i}-\xi^{i},

since Φ(0)=Il\Phi(0)=I_l (the identity matrix; degenerate interval by the convention of Mean-Square Riemann Integral of a Family of Random Variables).

Group 2 (time-integral part). For fixed j′′j'', set Hu=∑j′′′Ψj′′j′′′(u)guj′′′H_u=\sum_{j'''}\Psi_{j''j'''}(u)g^{j'''}_u (mean-square continuous by claims 1-2 of Basic Properties of the Mean-Square Riemann Integral); by claim 1 there, Yuj′′=∫0uHv dvY^{j''}_u=\int_0^uH_v\,dv almost surely, the two expressions for Yj′′Y^{j''} agreeing at each time. Apply part 2 of Integration by Parts for Wiener Integrals and Mean-Square Riemann Integrals with f=Φij′′f=\Phi_{ij''}, g=(AΦ)ij′′g=(A\Phi)_{ij''}:

∫0tΦij′′(u)Hu du+∫0t(AΦ)ij′′(u) Yuj′′ du=Φij′′(t) Ytj′′.\int_0^t\Phi_{ij''}(u)H_u\,du+\int_0^t(A\Phi)_{ij''}(u)\,Y^{j''}_u\,du=\Phi_{ij''}(t)\,Y^{j''}_t .

Summing over j′′j'' and using ∑j′′Φij′′(u)Ψj′′j′′′(u)=(ΦΨ)ij′′′(u)=δij′′′\sum_{j''}\Phi_{ij''}(u)\Psi_{j''j'''}(u)=(\Phi\Psi)_{ij'''}(u)=\delta_{ij'''} (claim 2 of Fundamental Solution and Variation of Constants for Linear Ordinary Differential Equations), the first sum collapses to ∫0tgui du\int_0^tg^{i}_u\,du; hence

∑j′′∫0t(AΦ)ij′′(u) Yuj′′ du=(Φ(t)Yt)i−∫0tgui du.\sum_{j''}\int_0^t(A\Phi)_{ij''}(u)\,Y^{j''}_u\,du=\bigl(\Phi(t)Y_t\bigr)^{i}-\int_0^tg^{i}_u\,du .

Group 3 (Wiener part). For each pair (j′′,j′)(j'',j') write Vuj′′j′=∫0u(Ψε)j′′j′ dWj′V^{j''j'}_u=\int_0^u(\Psi\varepsilon)_{j''j'}\,dW^{j'}. Part 1 of Integration by Parts for Wiener Integrals and Mean-Square Riemann Integrals with f=Φij′′f=\Phi_{ij''}, g=(AΦ)ij′′g=(A\Phi)_{ij''}, k=(Ψε)j′′j′k=(\Psi\varepsilon)_{j''j'} gives

∫0tΦij′′(u)(Ψε)j′′j′(u) dWuj′=Φij′′(t) Vtj′′j′−∫0t(AΦ)ij′′(u) Vuj′′j′ du.\int_0^t\Phi_{ij''}(u)(\Psi\varepsilon)_{j''j'}(u)\,dW^{j'}_u=\Phi_{ij''}(t)\,V^{j''j'}_t-\int_0^t(A\Phi)_{ij''}(u)\,V^{j''j'}_u\,du .

Summing over j′′j'' (Wiener-integral linearity for the left side) gives, for each j′j', the integrand ∑j′′Φij′′(Ψε)j′′j′=(ΦΨε)ij′=εij′\sum_{j''}\Phi_{ij''}(\Psi\varepsilon)_{j''j'}=(\Phi\Psi\varepsilon)_{ij'}=\varepsilon_{ij'}; then summing over j′j',

∑j′′∫0t(AΦ)ij′′(u) Zuj′′ du=(Φ(t)Zt)i−∑j′∫0tεij′(u) dWuj′.\sum_{j''}\int_0^t(A\Phi)_{ij''}(u)\,Z^{j''}_u\,du=\bigl(\Phi(t)Z_t\bigr)^{i}-\sum_{j'}\int_0^t\varepsilon_{ij'}(u)\,dW^{j'}_u .

Assembly. Adding the three groups and ∫0tgi du\int_0^tg^{i}\,du:

∫0t(∑jAijXrj+gri)dr=(Φ(t)(ξ+Yt+Zt))i−ξi−∑j′∫0tεij′ dWuj′=Xti−ξi−∑j′∫0tεij′ dWuj′,\int_0^t\Bigl(\sum_jA_{ij}X^{j}_r+g^{i}_r\Bigr)dr=\bigl(\Phi(t)(\xi+Y_t+Z_t)\bigr)^{i}-\xi^{i}-\sum_{j'}\int_0^t\varepsilon_{ij'}\,dW^{j'}_u=X^{i}_t-\xi^{i}-\sum_{j'}\int_0^t\varepsilon_{ij'}\,dW^{j'}_u ,

which is the equation of Mean-Square Solution of a Linear Stochastic Differential Equation with Additive Wiener Noise, rearranged.

Claim 2. Let X,X~X,\widetilde X be mean-square solutions and put v(t)=∑i∥Xti−X~ti∥2v(t)=\sum_i\lVert X^{i}_t-\widetilde X^{i}_t\rVert_2, a continuous function (claim 4 of Basic Properties of the Mean-Square Riemann Integral applied to the difference families, which are mean-square continuous). Subtracting the two defining equations (the ξ\xi, gg, and Wiener terms cancel), Xti−X~ti=∫0t∑jAij(r)(Xrj−X~rj) drX^{i}_t-\widetilde X^{i}_t=\int_0^t\sum_jA_{ij}(r)(X^{j}_r-\widetilde X^{j}_r)\,dr almost surely, so by the norm bound (claim 4 of Basic Properties of the Mean-Square Riemann Integral) and the entry bound ∣Aij∣≤α|A_{ij}|\le\alpha,

∥Xti−X~ti∥2≤∫0tα v(r) dr,hencev(t)≤lα∫0tv(r) dr(0≤t≤T).\lVert X^{i}_t-\widetilde X^{i}_t\rVert_2\le\int_0^t\alpha\,v(r)\,dr,\qquad\text{hence}\qquad v(t)\le l\alpha\int_0^tv(r)\,dr\qquad(0\le t\le T).

By Gronwall's Lemma (Integral Form) (with constants 00 and lαl\alpha; the interval is already of the form [0,T][0,T]), v≤0v\le0; since v≥0v\ge0, v≡0v\equiv0, and the null-equivalence of Square-Integrable Random Variables and the Mean-Square Inner Product gives Xti=X~tiX^{i}_t=\widetilde X^{i}_t almost surely.

Claim 3. Write S\mathcal{S} for the closed mean-square span of the collection {ξj}∪{grj:r≤t}∪{Wrj′:r≤t}\{\xi^{j}\}\cup\{g^{j}_r:r\le t\}\cup\{W^{j'}_r:r\le t\}; by claim 1 of The Closed Mean-Square Span of a Family of Random Variables, S\mathcal{S} is closed under finite linear combinations and mean-square limits and contains the collection. First, Ytj∈SY^{j}_t\in\mathcal{S}: it is a finite sum of mean-square Riemann integrals over [0,t][0,t], each a mean-square limit of its mean-square Riemann sums (Mean-Square Riemann Integral of a Family of Random Variables), which are finite linear combinations of values Ψjj′′(τ)gτj′′\Psi_{jj''}(\tau)g^{j''}_\tau with τ≤t\tau\le t — scalar multiples of members of the collection. Second, Ztj∈SZ^{j}_t\in\mathcal{S}: each Wiener integral ∫0t(Ψε)jj′ dWj′\int_0^t(\Psi\varepsilon)_{jj'}\,dW^{j'} is, by claim 1 of Adapted Mean-Square Continuous Processes are Ito Integrable and claim 1 of Existence and Uniqueness of the Mean-Square Extension of the Elementary Stochastic Integral, a mean-square limit of elementary stochastic integrals of simple approximants taking the deterministic grid values of the integrand; each such elementary integral is a finite linear combination of increments Wtp+1j′−Wtpj′W^{j'}_{t_{p+1}}-W^{j'}_{t_p} with tp≤tt_p\le t, hence of members of the collection. Finally Xti=∑jΦij(t)(ξj+Ytj+Ztj)X^{i}_t=\sum_j\Phi_{ij}(t)(\xi^{j}+Y^{j}_t+Z^{j}_t) is a finite linear combination of members of S\mathcal{S}, hence lies in S\mathcal{S}; this is claim 3. ■\blacksquare

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