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Riemann--Fubini on product rectangles, with lower and upper section integrals and content-zero exceptional sections

Statement

Let ARpA\subseteq\mathbb R^p and BRqB\subseteq\mathbb R^q be nondegenerate closed rectangles, and let f:A×BRf:A\times B\to\mathbb R be Riemann integrable. Then the four lower and upper section-integral functions of Sections, lower and upper section integrals, and iterated Riemann integrals on product rectangles and Jordan sets are Riemann integrable and AB=AuB=A×Bf=BA=BuA.\int_A\ell_B=\int_Au_B=\int_{A\times B}f=\int_B\ell_A=\int_Bu_A.

If the BB-sections are integrable outside a content-zero set NAN\subseteq A, every bounded exceptionally completed function hh with h(x)=Bfxh(x)=\int_Bf_x for xNx\notin N is integrable and A×Bf=Ah.\int_{A\times B}f=\int_Ah. The same assertion holds with the coordinate blocks exchanged. In particular, when every section in an order is integrable, the ordinary iterated integral in that order exists and equals the multiple integral. The theorem does not assert that every section of an integrable function is integrable.

Facts & Assumptions

Given: Nondegenerate rectangles A,BA,B and a Riemann-integrable f:A×BRf:A\times B\to\mathbb R.

[L1]

Product-grid Darboux sums bound the outer Darboux sums of the lower and upper section-integral functions (A product grid bounds the Darboux sums of the lower and upper section-integral functions).

[L2]

A bounded f:QRf:Q\to\mathbb R on a nondegenerate rectangle is Riemann integrable if and only if, for every ε>0\varepsilon>0, some grid PP satisfies U(f,P)L(f,P)<εU(f,P)-L(f,P)<\varepsilon (Riemann's criterion on a nondegenerate rectangle in Rm\mathbb{R}^m: integrability is equivalent to arbitrarily small Darboux gaps).

[L3]

A content-zero set has finite cube covers of arbitrarily small total volume (Measure zero and content zero in Rm\mathbb{R}^m by countable and finite cube covers).

Proof

technique · direct
1.1

Given ε>0\varepsilon>0, [L2] supplies a grid of A×BA\times B with Darboux gap below ε\varepsilon. Its coordinate grids form a product grid, and [L1] places the lower and upper Darboux gaps of both B\ell_B and uBu_B inside that same gap.

L1L2given
2.1

By [L2], both B\ell_B and uBu_B are integrable. The inequalities in [L1], applied to grids with gaps tending to zero, give ABA×Bf\int_A\ell_B\ge\int_{A\times B}f and AuBA×Bf\int_Au_B\le\int_{A\times B}f; since BuB\ell_B\le u_B, all three values are equal. The same argument after exchanging AA and BB gives the other two equalities.

L2step 1.1algebra
3.1

Suppose h=Bfxh=\int_Bf_x outside a content-zero NN. There h=B=uBh=\ell_B=u_B. If MM bounds h,B,uB|h|,|\ell_B|,|u_B|, a finite cube cover of NN with arbitrarily small total volume, refined into an outer grid, bounds the upper integral of hB|h-\ell_B| by 2M2M times that volume. The criterion [L2] therefore makes hBh-\ell_B integrable with integral 00, and linearity gives Ah=AB=A×Bf\int_Ah=\int_A\ell_B=\int_{A\times B}f. The exchanged assertion is identical.

L2L3L4step 2.1algebra

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