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Loomis–Whitney integral inequality

Statement

Assume Countable Choice. Let n≥2. For each i∈{1,…,n} let gi:Rn−1→[0,∞) be Lebesgue-measurable and integrable, with its arguments identified with all coordinates except xi. Then ∫Rn∏i=1ngi(x1,…,xi^,…,xn)1/(n−1) dx≤∏i=1n(∫Rn−1gi)1/(n−1).

Facts & Assumptions

Given: Countable Choice and an integer n≥2 and nonnegative integrable functions gi on the coordinate hyperplanes.

[F1]

Tonelli applies to nonnegative product-measurable functions on sigma-finite measure spaces. Under Countable Choice, Euclidean Lebesgue measure is the completion of each product of its coordinate factors. In particular Borel functions on a Euclidean product are product-measurable and their product integrals equal their Euclidean integrals. (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product, The Euclidean Lebesgue measure is the completion of the product of the factor Lebesgue measures)

[F3]

Under Countable Choice, Lebesgue measure is the completion of its Borel restriction, and every completion-measurable function has a base-measurable representative. Thus each nonnegative finite Lebesgue-measurable gi has a nonnegative finite Borel representative equal almost everywhere. (L(Rn) is exactly the completion of the restriction of λn to the Borel sets, A function measurable for a completion is almost everywhere equal to one measurable for the original sigma-algebra)

[A2]

Countable Choice is used in the Borel-representative and Euclidean-product identification suppliers. No unqualified choice-free Lebesgue product identity is asserted. (The Axiom of Countable Choice (ACω))

[F2]

For nonnegative integrable functions, Hölder's inequality bounds the integral of a product by the product of the corresponding norms. (Holder's inequality for integrals, including the endpoint cases)

[A1]

For the induction step in dimension n≥3, assume the inequality in dimension n−1.

Proof

Given: Countable Choice, the integer n and nonnegative integrable coordinate functions gi.

1.1A2F1F3givenbase

First replace the gi by their Borel representatives from [F3], setting each representative to zero on its Borel set of nonfinite or negative values. The exceptional sets lie in Borel null sets Ni. Their coordinate lifts are null in Rn: intersect Ni×R with slabs Ni×[−k,k], k≥1, and apply the product rectangle formula in [F1], then take their countable union and permute coordinates. Completeness in [F1] therefore makes the original product Lebesgue-measurable with the same integral as the Borel product; the right-hand integrals are unchanged as well. We may henceforth assume all inputs Borel. For n=2, Tonelli [F1] factors the left side as (∫Rg1)(∫Rg2), which is the right side.

2.1A1F1F2step 1.1givenIH

For n≥3, assume [A1]. For i<n define hi(x1,…,xi^,…,xn−1):=∫Rgi(x1,…,xi^,…,xn−1,xn) dxn. Apply Tonelli [F1] using the Borel sigma-algebras: each hi is Borel and integrable, possibly infinite on a Borel null set. Set it to zero there. The lifted exceptional sets in Rn−1 are null by the slab argument of step 1.1. Consequently all the following sectional inequalities hold almost everywhere, and the modified hi are admissible finite inputs for [A1]. Applying Hölder [F2] in xn to the first n−1 factors and then Tonelli gives an upper bound for the left side of ∫Rn−1gn(x′)1/(n−1)∏i<nhi(xi^′)1/(n−1) dx′. Set H(x′):=∏i<nhi(xi^′)1/(n−2). Hölder in x′ with exponents (n−1)/(n−2) and n−1 bounds this by (∫H)(n−2)/(n−1)(∫gn)1/(n−1). The induction hypothesis [A1] bounds ∫H≤∏i<n(∫hi)1/(n−2), while Tonelli gives ∫hi=∫gi. Substitution yields the claimed product bound in dimension n.

3.1step 1.1step 2.1discharge-induction: step 2.1∎

Induction from the base case [step 1.1] through step 2.1 proves the inequality for every integer n≥2.

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