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TheoremStatement: AI-adaptedProof: AI-generatedverified 2026-09-26 (gpt-6-sol)
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Polar coordinates decompose Lebesgue measure into r^{n-1} dr d sigma

Statement

Assume the Axiom of Countable Choice (The Axiom of Countable Choice (ACω)). Let n≥1, let Sn−1⊆Rn be the unit sphere, and let σ be the set function of The polar surface set function on the unit sphere. Then σ is a finite Borel measure on Sn−1, and for every Borel measurable f:Rn→[0,∞], ∫Rnf(x) dλn(x)=∫0∞∫Sn−1f(rω)rn−1 dσ(ω) dr. Moreover, σ is the unique Borel measure on Sn−1 with this property.

Facts & Assumptions

Given: The Axiom of Countable Choice, a positive integer n, and a Borel measurable function f:Rn→[0,∞].

[L1]

The set function σ is defined by σ(E)=n λn({rω:ω∈E, 0<r≤1}) for Borel E⊆Sn−1. (The polar surface set function on the unit sphere)

[L3]

Two measures that agree on a sigma-finite generating pi-system agree on the generated sigma-algebra. (Measures agreeing on a generating pi-system are equal under an increasing finite-measure exhaustion from that pi-system)

[L4]

Tonelli's theorem turns equality of measures on sets into the corresponding equality of nonnegative integrals. (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product)

[L5]

Assuming countable choice, bounded subsets of Euclidean space have finite outer measure. (Lebesgue measure is sigma-finite, and every metrically bounded subset of Rn has finite outer measure)

[A1]

Let Φ:Rn∖{0}→(0,∞)×Sn−1 be Φ(x)=(∣x∣,x/∣x∣). This map is continuous, so m∗(B):=λn(Φ−1(B)) defines a measure on the Borel subsets of (0,∞)×Sn−1.

[A2]

Sets of the form (a,b]×E with 0<a<b and Borel E⊆Sn−1 form a sigma-finite generating pi-system for the Borel sigma-algebra of (0,∞)×Sn−1.

Proof

technique · direct
1.1L1L5A1

For Borel E⊆Sn−1 put Er:={sω:ω∈E, 0<s≤r}. By [A1], each Er is Borel. If (Ej) is pairwise disjoint, then the sets (Ej)1 are pairwise disjoint and (⋃jEj)1=⋃j(Ej)1, so countable additivity of λn makes σ a Borel measure. It is finite because σ(Sn−1)=nλn({x:0<∣x∣≤1})<∞ by [L5].

2.1L1L2A1step 1.1

For Borel E⊆Sn−1 and 0<a<b, [L1] gives λn(E1)=σ(E)/n. The dilation x↦rx has determinant rn, so [L2] gives λn(Er)=rnλn(E1)=rnnσ(E). Therefore m∗((a,b]×E)=λn(Eb∖Ea)=bn−annσ(E)=σ(E)∫abrn−1 dr.

3.1A2L3L4step 1.1step 2.1∎

Step 2.1 shows that m∗ and the product measure rn−1dr×σ agree on the generating pi-system of [A2]. The rectangles Pk=(1/k,k]×Sn−1 for k≥2 increase to the whole product and have the same finite measure under both measures, namely σ(Sn−1)(kn−k−n)/n; hence [L3] applies and the measures agree on every Borel subset of (0,∞)×Sn−1. Applying [L4] to this identity gives the integral formula on Rn∖{0}. The omitted origin has Lebesgue measure zero: it lies in a half-open box of volume εn for every ε>0. Thus the same formula holds for every nonnegative Borel measurable f on all of Rn, even when f(0)=+∞. If σ~ is another Borel measure on Sn−1 with the same integral formula, apply that formula to 1E1, where E1={rω:ω∈E, 0<r≤1}. Then λn(E1)=∫0∞∫Sn−11E1(rω)rn−1 dσ~(ω) dr=σ~(E)∫01rn−1 dr=σ~(E)n, so σ~(E)=nλn(E1)=σ(E) by [L1]. Thus σ~=σ, proving uniqueness.

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