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Mixed-derivative bounds for dyadic Simpson details

Statement

Use the dyadic composite-Simpson hierarchy of Nested one-dimensional quadrature levels and differences. Let d≥1. For S={j1<⋯<jk}⊆{1,…,d}, define DSf:=∂xjk4⋯∂xj14f, so these derivatives are applied in increasing coordinate order; set D∅f=f. Assume every DSf is continuous on the closed cube, with the one-sided endpoint convention of Higher derivatives and the classes Ck and C∞, and choose finite bounds MS≥0 such that ∣DSf(x)∣≤MS on [0,1]d. For ℓ∈N0d, put S(ℓ):={j:ℓj≥1} and δℓ(f):=(Δℓ1(1)⊗⋯⊗Δℓd(d))(f). Then ∣δℓ(f)∣≤MS(ℓ)(172880)∣S(ℓ)∣16−∑j∈S(ℓ)ℓj. Moreover, for every finite F⊆N0d, ∑ℓ∈F∣δℓ(f)∣≤∑S⊆{1,…,d}MS(1743200)∣S∣<∞.

Facts & Assumptions

Given: d≥1 and a function with the continuous mixed fourth partials and finite bounds stated above.

[F1]

Nested one-dimensional quadrature levels and differences: Qℓ=QS(⋅;0,1,2ℓ+1), Δ0=Q0, and Δℓ=Qℓ−Qℓ−1 for ℓ≥1.

[F2]

Composite Simpson error bound for a four-times continuously differentiable function: on [0,1], for an even panel count N≥2, ∣∫01g−QS(g;0,1,N)∣≤(180N4)−1∥g(4)∥∞ for g∈C4[0,1].

[F3]

Composite Simpson rule on an even uniform grid: the two-panel level-zero rule has nonnegative weights 1/6,4/6,1/6, which sum to one.

[F4]

Higher derivatives and the classes Ck and C∞: the stated continuous mixed derivatives exist through the required coordinatewise orders, with one-sided endpoint derivatives.

[F5]

Triangle inequality for finite sums: the absolute value of a finite sum is at most the sum of its absolute values.

[F6]

Laws of finite sums and finite products: finite sums may be regrouped and distribute over products, and are monotone in their terms.

[F7]

For ∣r∣<1, ∑k≥0rk=1/(1−r), and for ∣r∣≥1 the series diverges states the series starting at k=0: for ratio 1/16, ∑k≥0(1/16)k=16/15. By Laws of integer exponents, (1/16)k=16−k. Removing the k=0 term, which is 1, gives ∑r≥116−r=1/15; since all terms are nonnegative, every finite partial sum starting at r=1 is at most 1/15.

Proof

1.1givenF1F2F3F5algebra

For ℓ≥1, use [F2] on levels ℓ and ℓ−1, inserting the exact integral between their values. With panel counts 2ℓ+1 and 2ℓ, [F5] gives ∣Δℓg∣≤(2−4(ℓ+1)/180+2−4ℓ/180)∥g(4)∥∞=(17/2880)16−ℓ∥g(4)∥∞. For ℓ=0, [F3] gives ∣Δ0g∣=∣Q0g∣≤∥g∥∞.

2.1givenF1F4step 1.1F6algebra

Apply the one-dimensional bounds successively in the coordinates. A finite quadrature functional commutes with derivatives in any other coordinate because it is a finite weighted sum. In each active coordinate j, apply step 1.1 to the section after the earlier-coordinate derivatives have been taken; the needed fourth derivative is the corresponding sequential mixed derivative. In each inactive coordinate use the level-zero supremum bound. Multiplying the bounds gives MS(ℓ)(17/2880)∣S(ℓ)∣16−∑j∈S(ℓ)ℓj. The stated continuous mixed derivatives justify each section estimate, and [F6] justifies the finite tensor expansions.

3.1givenstep 2.1F6F7algebra∎

Fix finite F and group indices by S=S(ℓ). For a fixed nonempty S, enlarge its levels to the finite box 1≤ℓj≤Rj where Rj is the largest such coordinate level in that group. By step 2.1 and [F6], the sum over that box is at most MS∏j∈S((17/2880)∑r=1Rj16−r)≤MS(17/43200)∣S∣, using [F7]. For S=∅, the only possible index is 0 and its term is at most M∅. Summing over all subsets proves the finite-subsum claim; the right side is finite.

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