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Strong order one for scalar and commutative-noise Milstein schemes

Statement

Assume AC. Let d,m≥1 be finite, let W be an m-dimensional Brownian motion relative to a filtration satisfying Continuous Brownian Ito processes, and let X solve dXt=b(Xt)dt+∑j=1mσj(Xt)dWtj,X0∈L2(Rd). Assume b,σ1,…,σm∈Cb3(Rd) as defined in Milstein updates, iterated Brownian integrals, and commutative noise. Put Lif=Df σi and assume commutative noise Liσj=Ljσi for all i,j. On the uniform grid tn=nh, h=T/N≤1, initialize Y0=X0 and use the product-increment Milstein update in the Definition. Then there is a constant CT, independent of N, such that max⁡0≤n≤NE∣Yn−Xtn∣2≤CTh2. Thus the grid root-mean-square error is O(h) on [0,T]. For m=1 the commutativity condition is automatic and the scheme is the scalar Milstein update. No claim is made for a noncommuting-noise scheme without an area sampler satisfying a separately proved approximation bound.

Facts & Assumptions

Given: AC, the SDE and coefficient hypotheses, a finite horizon T>0, an integer N≥1 with h=T/N≤1, the exact solution X, and the Milstein grid process Y.

[L1]

Milstein updates, iterated Brownian integrals, and commutative noise: the commutative update is Yn+1=Yn+b(Yn)h+∑jσj(Yn)ΔWnj+12∑i,jLiσj(Yn)(ΔWniΔWnj−δijh).

[L2]

Product identity and conditional moments for iterated Brownian integrals: Iij,n+Iji,n=ΔWniΔWnj−δijh, so the commutative double-integral term equals the product-increment term.

[L3]

Conditional local defect bounds for the Milstein Taylor increment: on each step, Xtn+1=Xtn+b(Xtn)h+∑jσj(Xtn)ΔWnj+∑i,jLiσj(Xtn)Iij,n+Rn+1, with ∣E[Rn+1∣Ftn]∣≤Ch2 and E[∣Rn+1∣2∣Ftn]≤Ch3.

[L4]

Discrete stochastic local-to-global RMS stability bound: if a grid error has an adapted Lipschitz drift increment, martingale-difference terms with variance O(h∣en∣2), a bounded local mean O(h2), and a centered local remainder with second moment O(h3), then its terminal and grid root-mean-square error is O(h).

[F1]

Continuous Brownian Ito processes: the Brownian increments after tn are independent of Ftn, and the SDE solution has the stated adapted continuous drift-plus-It^o decomposition.

[A1]

The Axiom of Choice: AC is inherited from the exact Brownian and It^o suppliers [F1], [L2], and [L3]; no choice is made in the error recurrence.

Proof

Given: The assumptions above.

1.1F1L1L2L3given

Define en=Yn−Xtn. Apply [L3] to the exact solution on [tn,tn+1]. Using [L2] and commutativity, the exact Taylor increment has the same product form as the update [L1], except that its coefficients are evaluated at Xtn and it includes the remainder Rn+1.

1.2F1L1L3step 1.1

Subtract the exact update from [L1]. With un=b(Yn)−b(Xtn), set Mn+1=∑j(σj(Yn)−σj(Xtn))ΔWnj+12∑i,j(Liσj(Yn)−Liσj(Xtn))(ΔWniΔWnj−δijh). Then en+1=en+hun+Mn+1−Rn+1. The increments after tn are independent of Ftn by [F1]; their first moments vanish, and each centered quadratic factor has mean zero. Hence Mn+1 is orthogonal to every square-integrable Ftn-measurable vector.

2.1F1L1step 1.2algebra

The derivatives of b are bounded, so ∣un∣≤C∣en∣. Also each Liσj is globally Lipschitz: its derivative is a sum of products of first and second derivatives of the diffusion fields, all bounded by [L1]. The linear Gaussian term in Mn+1 has conditional second moment at most Ch∣en∣2. For the quadratic term, E[(ΔWiΔWj−δijh)2∣Ftn]≤2h2 by independent centered normal coordinates; the finite sum and the Lipschitz bound therefore give second moment at most Ch2∣en∣2≤Ch∣en∣2. Thus E∣Mn+1∣2≤Ch E∣en∣2.

2.2L3L4step 1.2algebra

Let rn=E[Rn+1∣Ftn] and Qn+1=−(Rn+1−rn). By [L3], ∣rn∣≤Ch2, E∣Rn+1∣2≤Ch3, and hence E∣Qn+1∣2≤2E∣Rn+1∣2+2E∣rn∣2≤Ch3 because h≤1. The defining event-integral property of conditional expectation makes Qn+1 orthogonal to every square-integrable Ftn-measurable vector. Therefore the recurrence in step 1.2 has the form required by [L4], with local mean −rn and centered terms Mn+1,Qn+1.

3.1A1L4step 2.2given∎

Initially e0=0. For each n≤N, apply [L4] to the recurrence restricted to the first n steps; its constants are the same because nh≤T. Thus max⁡0≤n≤NE∣en∣2≤CTh2, and taking square roots gives the stated grid root-mean-square order one. When m=1, the only commutativity equation is L1σ1=L1σ1; if all diffusion fields vanish, the stochastic terms and their bounds vanish and the same proof reduces to the deterministic recurrence. The argument uses AC only through [A1].

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