Fix the component index i and abbreviate the modulus of continuity: by Continuity on a Closed Interval Implies Uniform Continuity choose ωn→0 bounding ∣fij(v)−fij(v′)∣ for all entries j and all v,v′∈[0,t] with ∣v−v′∣≤t/n. Norms 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.
Claim 1. By claim 5 of Basic Properties of the Mean-Square Riemann Integral and the interval-splitting of Wiener integrals (Ito Integrable Process and the Ito Integral, claim 1 of Properties of the Ito Integral: Linearity, Isometry, Martingale Property, and Mean-Square Continuity), almost surely,
uxpj−uxp−1j=∫xp−1xp(E~X)vjdv+j′∑(∫0xpε~jj′dWj′−∫0xp−1ε~jj′dWj′).
Hence the i-th component of the Riemann-Stieltjes sum splits into a time part ∑p∑jfij(xp−1)∫xp−1xp(E~X)vjdv and a Wiener part.
Time part. By claims 1, 2, 5 of Basic Properties of the Mean-Square Riemann Integral (with the n-fold split of ∫0t obtained by induction from claim 5), the difference from ∫0t(fE~X)vidv equals ∑p∑j∫xp−1xp(fij(xp−1)−fij(v))(E~X)vjdv, whose norm is at most ωn∑j∫0t∥(E~X)vj∥2dv→0 by the norm bound (claim 4 there).
Wiener part. Fix j′. With Vsjj′:=∫0sε~jj′dWj′, the relevant difference is
Dn=p∑j∑fij(xp−1)(Vxpjj′−Vxp−1jj′)−∫0t(fε~)ij′(v)dWvj′.
All terms are Wiener integrals of continuous functions against Wj′, members of the centered jointly Gaussian family of claims 2-3 of Wiener Integrals Against a Vector Brownian Motion are Jointly Gaussian, so E[Dn2] is a finite bilinear combination of the covariances given by claim 3 there: increments Vxpjj′−Vxp−1jj′ and Vxqj′′j′−Vxq−1j′′j′ over disjoint cells p=q are uncorrelated (evaluate the four min terms), while over the same cell Cov(Vxpjj′−Vxp−1jj′,Vxpj′′j′−Vxp−1j′′j′)=∫xp−1xpε~jj′ε~j′′j′dv and Cov(Vxpjj′−Vxp−1jj′,∫0t(fε~)ij′dWj′)=∫xp−1xpε~jj′(fε~)ij′dv (Additivity of the Riemann Integral on Adjacent Intervals for the interval splittings). Writing sn(v)=∑jfij(xp(v)−1)ε~jj′(v), where p(v) is the index with v∈(xp(v)−1,xp(v)] (so sn depends on i and j′), collecting the three groups of terms and completing the square in each cell yields
E[Dn2]=p∑∫xp−1xp(sn(v)−(fε~)ij′(v))2dv≤t(l~ωnmax∣ε~∣)2→0,
since ∣sn(v)−(fε~)ij′(v)∣=∣∑j(fij(xp(v)−1)−fij(v))ε~jj′(v)∣≤l~ωnmax∣ε~∣, with max∣ε~∣ a bound on all entries of ε~ (Extreme Value Theorem on a Compact Interval); monotonicity of the Riemann integral is via Agreement of the Riemann and Lebesgue Integrals for Continuous Functions on a Closed Interval and Linearity and Monotonicity of the Lebesgue Integral. Summing the two parts over the finitely many indices (triangle inequality) proves claim 1.
Claim 2. Each Riemann-Stieltjes sum is a finite linear combination of the values uxpj with xp≤t, all Gt-measurable. By claim 1 the sums converge in mean square to the component of ∫0tfdu, so that component lies in the closed mean-square span of the values urj (r≤t) — the second assertion — and, by claim 2 of The Closed Mean-Square Span of a Family of Random Variables applied with G=Gt, it is almost surely equal to a Gt-measurable square-integrable random variable. ■