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Shared-Brownian Euler level correction rates

Statement

Assume AC and the finite-L2 coefficient and initial-value hypotheses of Euler–Maruyama strong rate for square-integrable initial data. Fix an integer refinement factor M≥2 and a fine step h with 0<h≤1/M, T/h∈N, and T/(Mh)∈N. Construct the fine and coarse Euler paths with the same initial value and Brownian motion. The coarse Brownian increment over each coarse interval is, by definition, the sum of the M fine Brownian increments in that interval. Let XT be the common exact solution, and let φ:Rd→R be globally Lipschitz with constant Lφ. Then constants independent of h satisfy E∣YTh−YTMh∣2≤CMh, Var⁡(φ(YTh)−φ(YTMh))≤CMLφ2h,∣Eφ(XT)−Eφ(YTh)∣≤CLφh1/2. Thus the Lipschitz-payoff Euler level pair has correction variance exponent β=1 and strong-error bias exponent α=1/2. If, in addition, φ is bounded and its backward value function satisfies the hypotheses of Euler–Maruyama weak order one under backward regularity, then the bias bound improves to ∣Eφ(XT)−Eφ(YTh)∣≤Ch, so α=1 while β=1 remains. With fixed dimension, fixed M, and unit-cost coefficient and payoff evaluations, one coupled fine/coarse sample has work O(h−1).

Facts & Assumptions

Given: AC; the stated finite-L2 SDE assumptions; the fixed refinement factor and nested grids; a common exact solution and Brownian path; and the Lipschitz payoff (plus, for the weak branch, the bounded-payoff backward contract).

[F1]

Under the finite-L2 coefficient, time-modulus, Brownian and initial-value hypotheses, the continuous Euler path satisfies Esup⁡t≤T∣Xt−Yth∣2≤Ch, uniformly in 0<h≤1 with T/h∈N. Euler–Maruyama strong rate for square-integrable initial data

[F2]

For the weak-bias branch, retain finite d,m, the Euclidean/Frobenius norm convention and A:B=tr⁡(ATB), and the same finite-horizon, complete usual filtered Brownian and grid setup as in the Statement. Assume jointly Borel coefficients that are globally Lipschitz in state, have uniform linear growth, and satisfy the half-Hölder time modulus. Require an F0-measurable initial value independent of future Brownian increments with E∣X0∣p<∞ for finite real q≥0 and finite p≥2q+8 (using ∣x∣0=1), and uniform pointwise order-p moments of the exact solution, Euler interpolation, and Euler step process on [0,T]. The payoff is bounded Borel, and its backward value function u(t,x)=E[φ(XTt,x)], using the unique shifted strong solutions supplied by the global well-posedness theorem, satisfies u(T,x)=φ(x), (∂t+Lt)u=0 for Ltv=b(t,⋅)⋅∇v+12(σσT)(t,⋅):Dx2v, and continuous mixed derivatives ∂tjDxαu for 0≤j≤2, ∣α∣≤4, bounded by Cu(1+∣x∣q). Under this full contract of Euler–Maruyama weak order one under backward regularity, ∣Eφ(XT)−Eφ(YTh)∣≤Ch.

[A1]

The refinement factor M is fixed as h→0; both mesh sizes obey 0<h≤1 and have T/h and T/(Mh) integral. The coarse path uses the sum of each corresponding block of M fine Brownian increments, so both Euler paths use the same Brownian path and initial value.

[A2]

∣φ(x)−φ(y)∣≤Lφ∣x−y∣ for all states. In the weak branch, the same φ is bounded and satisfies the additional backward regularity contract [F2].

[A3]

AC is included because [F1] carries that assumption from the Doob and Brownian Itô interfaces. The Axiom of Choice

Proof

Given: AC; the stated finite-L2 SDE assumptions; the fixed refinement factor and nested grids; a common exact solution and Brownian path; and the Lipschitz payoff (plus, for the weak branch, the bounded-payoff backward contract).

[F1] Under the finite-L2 coefficient, time-modulus, Brownian and initial-value hypotheses, the continuous Euler path satisfies Esup⁡t≤T∣Xt−Yth∣2≤Ch, uniformly in 0<h≤1 with T/h∈N. Euler–Maruyama strong rate for square-integrable initial data

[F2] For the weak-bias branch, retain finite d,m, the Euclidean/Frobenius norm convention and A:B=tr⁡(ATB), and the same finite-horizon, complete usual filtered Brownian and grid setup as in the Statement. Assume jointly Borel coefficients that are globally Lipschitz in state, have uniform linear growth, and satisfy the half-Hölder time modulus. Require an F0-measurable initial value independent of future Brownian increments with E∣X0∣p<∞ for finite real q≥0 and finite p≥2q+8 (using ∣x∣0=1), and uniform pointwise order-p moments of the exact solution, Euler interpolation, and Euler step process on [0,T]. The payoff is bounded Borel, and its backward value function u(t,x)=E[φ(XTt,x)], using the unique shifted strong solutions supplied by the global well-posedness theorem, satisfies u(T,x)=φ(x), (∂t+Lt)u=0 for Ltv=b(t,⋅)⋅∇v+12(σσT)(t,⋅):Dx2v, and continuous mixed derivatives ∂tjDxαu for 0≤j≤2, ∣α∣≤4, bounded by Cu(1+∣x∣q). Under this full contract of Euler–Maruyama weak order one under backward regularity, ∣Eφ(XT)−Eφ(YTh)∣≤Ch.

[A1] The refinement factor M is fixed as h→0; both mesh sizes obey 0<h≤1 and have T/h and T/(Mh) integral. The coarse path uses the sum of each corresponding block of M fine Brownian increments, so both Euler paths use the same Brownian path and initial value.

[A2] ∣φ(x)−φ(y)∣≤Lφ∣x−y∣ for all states. In the weak branch, the same φ is bounded and satisfies the additional backward regularity contract [F2].

[A3] AC is included because [F1] carries that assumption from the Doob and Brownian Itô interfaces. The Axiom of Choice

1.1F1A1algebra

By [A1], the fine and coarse paths are driven by nested increments of this common Brownian path. Since h≤1/M, both meshes lie in the range of [F1]. Therefore ∣YTh−YTMh∣2≤2∣YTh−XT∣2+2∣YTMh−XT∣2. Taking expectations and applying [F1] at step sizes h and Mh gives E∣YTh−YTMh∣2≤2Ch+2CMh=2C(1+M)h. This is the correction second-moment bound.

1.2A2F1algebra

The same Lipschitz bound and Cauchy–Schwarz give ∣Eφ(XT)−Eφ(YTh)∣≤LφE∣XT−YTh∣≤Lφ(E∣XT−YTh∣2)1/2≤C1/2Lφh1/2. Thus β=1 and the strong route gives α=1/2.

2.1A2step 1.1algebra

Let D=φ(YTh)−φ(YTMh). Since variance is at most second moment and [A2] gives ∣D∣≤Lφ∣YTh−YTMh∣, step 1.1 yields Var⁡(D)≤ED2≤2C(1+M)Lφ2h.

3.1F2step 2.1

If the additional bounded-payoff backward contract holds, [F2] applied to the same fine Euler scheme gives bias at most Ch. It changes only the bias exponent to α=1; the correction-variance bound of step 2.1 is unchanged.

4.1A1A3step 3.1∎

A fine path takes T/h Euler steps and the coarse path takes T/(Mh) steps. The coarse increments are sums of already generated fine increments, so they add no Brownian draws; for fixed M,d and unit-cost coefficient/payoff evaluations, total path work is proportional to T/h+T/(Mh)=O(h−1). AC is inherited only through [A3].

Remarks

This is the solver-rate interface for multilevel examples; it makes no claim about learned-drift or learned-score bias. The variance-rate and work statements do not import the abstract MLMC complexity theorem.

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