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A nonzero leading defect makes the embedded difference asymptotically match the low-order defect

Statement

Fix one initial value problem and initial state. Let Dp(h):=Y^(h)−y(t+h) be the low member's one-step defect and Dp+1(h):=Y(h)−y(t+h) the high member's defect, using the same exact initial state and step start. Suppose, as h↓0, Dp(h)=ahp+1+O(hp+2),Dp+1(h)=O(hp+2) for a fixed vector a∈Rd. Here O(hr) for a vector means a remainder whose Euclidean norm is at most Chr for all sufficiently small positive h. Then Y^(h)−Y(h)=ahp+1+O(hp+2). If a≠0, the estimator satisfies E(h)/∥Dp(h)∥2→1. If a=0, these hypotheses do not imply that this ratio tends to one or that the estimator is nonzero; the Euler–Heun pair on y′=t2, y(0)=0, has ratio 3/2 as computed below.

Facts & Assumptions

Given: The two outputs and Euclidean estimator in Embedded Runge–Kutta pair and difference estimator, with the two displayed defect expansions.

[F1]

Embedded Runge–Kutta pair and difference estimator: E(h)=∥Y^(h)−Y(h)∥2.

[F2]

Cauchy-Schwarz ∣⟨x,y⟩∣≤∥x∥2∥y∥2 with its equality case, the triangle inequality for ∥⋅∥2, the parallelogram law and polarisation: the Euclidean norm is continuous and satisfies ∣∥u∥2−∥v∥2∣≤∥u−v∥2.

[F3]

Euler–Heun embedded Runge–Kutta pair: Heun and Euler use the two shared stages K1=f(t,y) and K2=f(t+h,y+hK1), with outputs YE=y+hK1 and YH=y+h2(K1+K2).

Proof

1.1givenF1algebra

Subtracting the two defect identities cancels the common exact value: Y^−Y=Dp−Dp+1=ahp+1+O(hp+2). Thus there is a vector remainder r(h)=O(hp+2) with Y^−Y=hp+1(a+hr1(h)), where r1 is bounded for all sufficiently small positive h.

2.1F1F2F3step 1.1algebra∎

By [F2], ∣E(h)/hp+1−∥a∥2∣≤h∥r1(h)∥2→0. If a≠0, the same argument gives ∥Dp(h)∥2/hp+1→∥a∥2>0; dividing the two positive limits proves E(h)/∥Dp(h)∥2→1. If a=0, the expansions give only Dp=O(hp+2) and E=O(hp+2), with no lower bound. To verify that the ratio-one conclusion can fail for an actual embedded Runge–Kutta pair, use the Heun–Euler pair [F3] on y′=t2, y(0)=0: K1=0, K2=h2, YE=0, YH=h3/2, and the exact endpoint is h3/3. Thus D1=−h3/3, the estimator is h3/2, and their norm ratio is 3/2, while the h2 coefficient is zero. Conversely, for the zero field with zero initial state, both outputs and the estimator vanish identically, so no positive lower bound for the estimator follows either.

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