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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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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)jjdWj\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=jΦjj(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,

j0t(AΦ)ij(r)ξjdr=j(Φij(t)Φij(0))ξj=(Φ(t)ξ)iξi,\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 jj'', set Hu=jΨjj(u)gujH_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=0uHvdvY^{j''}_u=\int_0^uH_v\,dv almost surely, the two expressions for YjY^{j''} agreeing at each time. Apply part 2 of Integration by Parts for Wiener Integrals and Mean-Square Riemann Integrals with f=Φijf=\Phi_{ij''}, g=(AΦ)ijg=(A\Phi)_{ij''}:

0tΦij(u)Hudu+0t(AΦ)ij(u)Yujdu=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 jj'' and using jΦij(u)Ψjj(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 0tguidu\int_0^tg^{i}_u\,du; hence

j0t(AΦ)ij(u)Yujdu=(Φ(t)Yt)i0tguidu.\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 Vujj=0u(Ψε)jjdWjV^{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=Φijf=\Phi_{ij''}, g=(AΦ)ijg=(A\Phi)_{ij''}, k=(Ψε)jjk=(\Psi\varepsilon)_{j''j'} gives

0tΦij(u)(Ψε)jj(u)dWuj=Φij(t)Vtjj0t(AΦ)ij(u)Vujjdu.\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 jj'' (Wiener-integral linearity for the left side) gives, for each jj', the integrand jΦij(Ψε)jj=(ΦΨε)ij=εij\sum_{j''}\Phi_{ij''}(\Psi\varepsilon)_{j''j'}=(\Phi\Psi\varepsilon)_{ij'}=\varepsilon_{ij'}; then summing over jj',

j0t(AΦ)ij(u)Zujdu=(Φ(t)Zt)ij0tεij(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 0tgidu\int_0^tg^{i}\,du:

0t(jAijXrj+gri)dr=(Φ(t)(ξ+Yt+Zt))iξij0tεijdWuj=Xtiξij0tεijdWuj,\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)=iXtiX~ti2v(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), XtiX~ti=0tjAij(r)(XrjX~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 Aijα|A_{ij}|\le\alpha,

XtiX~ti20tαv(r)dr,hencev(t)lα0tv(r)dr(0tT).\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]), v0v\le0; since v0v\ge0, v0v\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:rt}{Wrj:rt}\{\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, YtjSY^{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 τt\tau\le t — scalar multiples of members of the collection. Second, ZtjSZ^{j}_t\in\mathcal{S}: each Wiener integral 0t(Ψε)jjdWj\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+1jWtpjW^{j'}_{t_{p+1}}-W^{j'}_{t_p} with tptt_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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