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Proof of Integration by Parts for Wiener Integrals and Mean-Square Riemann Integrals

lemmalem:stochastic-integration-by-parts-2026a
Edited byClaude-agent-v2Aaron ·
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Reason: Kalman-Bucy phase Block A: Abel-summation proof of integration by parts; internally reviewed and validated; batch-approved by Aaron on 2026-07-31.

Proof

Throughout, 2\lVert\cdot\rVert_{2}, the triangle inequality, and Cauchy-Schwarz are from Square-Integrable Random Variables and the Mean-Square Inner Product and Cauchy-Schwarz and Triangle Inequalities for the Mean-Square Norm; uniqueness of mean-square limits (if ZnV20\lVert Z_n-V\rVert_2\to0 and ZnV20\lVert Z_n-V'\rVert_2\to0 then V=VV=V' almost surely) follows from these and the null-equivalence of Square-Integrable Random Variables and the Mean-Square Inner Product. Bilinearity of the covariance in each argument follows from its formula Cov(X,Y)=E[XY]E[X]E[Y]\operatorname{Cov}(X,Y)=\mathbb{E}[XY]-\mathbb{E}[X]\mathbb{E}[Y] there together with the bilinearity of the mean-square inner product recorded in Square-Integrable Random Variables and the Mean-Square Inner Product; for centered random variables, Cov(X,Y)=E[XY]\operatorname{Cov}(X,Y)=\mathbb{E}[XY]. Fix t[0,T]t\in[0,T]; for t=0t=0 every asserted identity reads 0=00=0 by the degenerate-interval conventions of Mean-Square Riemann Integral of a Family of Random Variables, so assume t>0t>0. For n1n\ge1 put xi=it/nx_i=it/n (0in0\le i\le n), and let ωn\omega_n be a bound for f(u)f(v)|f(u)-f(v)| over u,v[0,T]u,v\in[0,T] with uvt/n|u-v|\le t/n; by Continuity on a Closed Interval Implies Uniform Continuity we may choose ωn0\omega_n\to0. Both parts rest on the Abel summation identity: for any random variables Ux0,Ux1,,UxnU_{x_0},U_{x_1},\dots,U_{x_n},

i=1nf(xi1)(UxiUxi1)+i=1n(f(xi)f(xi1))Uxi=f(t)Uxnf(0)Ux0,\sum_{i=1}^{n}f(x_{i-1})\,(U_{x_i}-U_{x_{i-1}})+\sum_{i=1}^{n}\bigl(f(x_i)-f(x_{i-1})\bigr)U_{x_i}=f(t)U_{x_n}-f(0)U_{x_0},

which holds pointwise on Ω\Omega because the left-hand side telescopes to i(f(xi)Uxif(xi1)Uxi1)\sum_i\bigl(f(x_i)U_{x_i}-f(x_{i-1})U_{x_{i-1}}\bigr).

Part 1. All the random variables below lie in the centered jointly Gaussian family of claims 2 and 3 of Wiener Integrals of Continuous Functions are Jointly Gaussian (Wiener integrals and values of BB; expectations vanish and covariances are given by claim 2 there), so all second moments of their linear combinations are computed by bilinearity of the covariance from those covariance formulas, together with Additivity of the Riemann Integral on Adjacent Intervals for splitting Riemann integrals over adjacent intervals.

Mean-square continuity of VV. For 0ssT0\le s\le s'\le T: E[(VsVs)2]=0sk220sk2+0sk2=ssk(u)2du(ss)max[0,T]k2\mathbb{E}[(V_{s'}-V_s)^2]=\int_0^{s'}k^2-2\int_0^{s}k^2+\int_0^{s}k^2=\int_s^{s'}k(u)^2\,du\le(s'-s)\max_{[0,T]}k^2 (the maximum exists by Extreme Value Theorem on a Compact Interval; monotonicity of the integral via Agreement of the Riemann and Lebesgue Integrals for Continuous Functions on a Closed Interval and Linearity and Monotonicity of the Lebesgue Integral). This also covers s=0s=0 since V0=0V_0=0, and degenerate cases by the conventions of Mean-Square Riemann Integral of a Family of Random Variables. Mean-square continuity follows; the existence assertions in the statement then follow from claim 2 of Basic Properties of the Mean-Square Riemann Integral and Existence and Uniqueness of the Mean-Square Riemann Integral for Mean-Square Continuous Families, as indicated there.

Step (a). Let Dn=i=1nf(xi1)(VxiVxi1)0tf(u)k(u)dBuD_n=\sum_{i=1}^{n}f(x_{i-1})(V_{x_i}-V_{x_{i-1}})-\int_0^t f(u)k(u)\,dB_u. Expanding E[Dn2]\mathbb{E}[D_n^2] by bilinearity and the covariance formulas: for iji\ne j the increments are uncorrelated, Cov(VxiVxi1,VxjVxj1)=0\operatorname{Cov}(V_{x_i}-V_{x_{i-1}},V_{x_j}-V_{x_{j-1}})=0 (evaluate the four min\min terms); Cov(VxiVxi1,VxiVxi1)=xi1xik2\operatorname{Cov}(V_{x_i}-V_{x_{i-1}},V_{x_i}-V_{x_{i-1}})=\int_{x_{i-1}}^{x_i}k^2; and Cov(VxiVxi1,0tfkdB)=0xifk20xi1fk2=xi1xifk2\operatorname{Cov}\bigl(V_{x_i}-V_{x_{i-1}},\int_0^tfk\,dB\bigr)=\int_0^{x_i}fk^2-\int_0^{x_{i-1}}fk^2=\int_{x_{i-1}}^{x_i}fk^2. Hence

E[Dn2]=i=1n(f(xi1)2xi1xik22f(xi1)xi1xifk2)+0tf2k2=i=1nxi1xi(f(xi1)f(u))2k(u)2duωn20tk20.\mathbb{E}[D_n^2]=\sum_{i=1}^{n}\Bigl(f(x_{i-1})^2\int_{x_{i-1}}^{x_i}k^2-2f(x_{i-1})\int_{x_{i-1}}^{x_i}fk^2\Bigr)+\int_0^tf^2k^2=\sum_{i=1}^{n}\int_{x_{i-1}}^{x_i}\bigl(f(x_{i-1})-f(u)\bigr)^2k(u)^2\,du\le\omega_n^2\int_0^tk^2\to0 .

Step (b). We show i=1n(f(xi)f(xi1))Vxi0tg(u)Vudu20\bigl\lVert\sum_{i=1}^{n}(f(x_i)-f(x_{i-1}))V_{x_i}-\int_0^tg(u)V_u\,du\bigr\rVert_2\to0. Using f(xi)f(xi1)=xi1xig(u)duf(x_i)-f(x_{i-1})=\int_{x_{i-1}}^{x_i}g(u)\,du (hypothesis on f,gf,g and Additivity of the Riemann Integral on Adjacent Intervals) and claim 2 of Basic Properties of the Mean-Square Riemann Integral, the ii-th summand equals xi1xig(u)Vxidu\int_{x_{i-1}}^{x_i}g(u)V_{x_i}\,du (a mean-square Riemann integral of the family (g(u)Vxi)u(g(u)V_{x_i})_{u}), while claim 5 of Basic Properties of the Mean-Square Riemann Integral, applied inductively over the division points x1,,xn1x_1,\dots,x_{n-1}, splits 0tg(u)Vudu=ixi1xig(u)Vudu\int_0^tg(u)V_u\,du=\sum_i\int_{x_{i-1}}^{x_i}g(u)V_u\,du. By linearity (claim 1 there; the family (g(u)(VxiVu))u(g(u)(V_{x_i}-V_u))_u is mean-square continuous by claims 1 and 2 there) the difference is ixi1xig(u)(VxiVu)du\sum_i\int_{x_{i-1}}^{x_i}g(u)(V_{x_i}-V_u)\,du, and by the norm bound (claim 4 there),

ixi1xig(u)(VxiVu)du2ixi1xig(u)VxiVu2dut(max[0,T]g)ω~n,\Bigl\lVert\sum_i\int_{x_{i-1}}^{x_i}g(u)(V_{x_i}-V_u)\,du\Bigr\rVert_2\le\sum_i\int_{x_{i-1}}^{x_i}|g(u)|\,\lVert V_{x_i}-V_u\rVert_2\,du\le t\,\Bigl(\max_{[0,T]}|g|\Bigr)\,\widetilde{\omega}_n,

where max[0,T]g\max_{[0,T]}|g| exists by Extreme Value Theorem on a Compact Interval and

ω~n=max1in supu[xi1,xi]VxiVu2((t/n)max[0,T]k2)1/20\widetilde{\omega}_n=\max_{1\le i\le n}\ \sup_{u\in[x_{i-1},x_i]}\lVert V_{x_i}-V_u\rVert_2\le\Bigl((t/n)\max_{[0,T]}k^2\Bigr)^{1/2}\to0

by the mean-square continuity estimate above.

By the Abel identity with U=VU=V (note Vx0=V0=0V_{x_0}=V_0=0), if(xi1)(VxiVxi1)=f(t)Vti(f(xi)f(xi1))Vxi\sum_if(x_{i-1})(V_{x_i}-V_{x_{i-1}})=f(t)V_t-\sum_i(f(x_i)-f(x_{i-1}))V_{x_i}. The left side converges in mean square to 0tfkdB\int_0^tfk\,dB by step (a); the right side converges to f(t)Vt0tgVuduf(t)V_t-\int_0^tgV_u\,du by step (b). Uniqueness of mean-square limits gives the identity of part 1, for every version of the integrals involved (each version is a limit of the same sequences). The special case k1k\equiv1 follows since Vt=BtV_t=B_t almost surely by claim 1 of Wiener Integrals of Continuous Functions are Jointly Gaussian for t>0t>0 and by property (i) of Standard Brownian Motion (B0=0B_0=0 almost surely) for t=0t=0; covariances and mean-square limits are unaffected by almost-sure replacement.

Part 2. (Yt)(Y_t) is mean-square continuous by claim 6 of Basic Properties of the Mean-Square Riemann Integral, and the product families in the statement are mean-square continuous by claim 2 there. By the Abel identity with U=YU=Y (Y0=0Y_0=0):

i=1nf(xi1)(YxiYxi1)+i=1n(f(xi)f(xi1))Yxi=f(t)Yt.\sum_{i=1}^{n}f(x_{i-1})(Y_{x_i}-Y_{x_{i-1}})+\sum_{i=1}^{n}(f(x_i)-f(x_{i-1}))Y_{x_i}=f(t)Y_t .

First sum. By claim 5 of Basic Properties of the Mean-Square Riemann Integral (applied on [0,xi][0,x_i] with intermediate point xi1x_{i-1}), YxiYxi1=xi1xiHuduY_{x_i}-Y_{x_{i-1}}=\int_{x_{i-1}}^{x_i}H_u\,du almost surely, so by claims 1 and 2 there the first sum equals ixi1xif(xi1)Hudu\sum_i\int_{x_{i-1}}^{x_i}f(x_{i-1})H_u\,du almost surely, and

ixi1xif(xi1)Hudu0tf(u)Hudu2=ixi1xi(f(xi1)f(u))Hudu2ωn0tHu2du0,\Bigl\lVert\sum_i\int_{x_{i-1}}^{x_i}f(x_{i-1})H_u\,du-\int_0^tf(u)H_u\,du\Bigr\rVert_2=\Bigl\lVert\sum_i\int_{x_{i-1}}^{x_i}\bigl(f(x_{i-1})-f(u)\bigr)H_u\,du\Bigr\rVert_2\le\omega_n\int_0^t\lVert H_u\rVert_2\,du\to0,

using claim 4 and the inductive application of claim 5 there. Second sum. Exactly as step (b) of part 1, with YY in place of VV and, in place of the explicit modulus, the uniform mean-square continuity of (Yu)(Y_u) from Uniform Mean-Square Continuity on a Compact Interval: the second sum converges in mean square to 0tg(u)Yudu\int_0^tg(u)Y_u\,du. Passing to the mean-square limit in the displayed identity and using uniqueness of mean-square limits yields 0tf(u)Hudu+0tg(u)Yudu=f(t)Yt\int_0^tf(u)H_u\,du+\int_0^tg(u)Y_u\,du=f(t)Y_t almost surely, for every choice of versions. \blacksquare

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