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Agreement with the existing polar sphere measure

Statement

Assume ACω and n≥2. The chart surface measure on Sn−1 equals the polar measure σ. Orthogonal transformations preserve it. The map ω↦a+Rω, R>0, multiplies surface measure by Rn−1, and ∣Sn−1∣=n∣B1∣.

Facts & Assumptions

Given: Assume ACω, n≥2. Compare the chart measure and existing polar measure on the unit sphere. For scaling take R>0 and a∈Rn.

[F1]

Chart integrals are independent of charts and partitions. (Chart and partition independence of surface measure).

[F2]

The polar formula holds for every nonnegative Borel function. (Polar coordinates decompose Lebesgue measure into r^{n-1} dr d sigma).

[F3]
[F4]

Increasing simple approximation justifies the separated product integration and passage from set measures to integrals. (Monotone convergence for the integral).

Proof

1.1givenF1algebra

Write m for chart measure and take a finite sphere atlas Xj:Uj→Sn−1 with a subordinate partition χj. Since ∣Xj∣2=1, differentiation gives Xj⋅∂iXj=0. For Tj(r,y)=rXj(y), 1<r<2, the derivative has columns Xj,r∂1Xj,…,r∂n−1Xj. Its Gram determinant is r2n−2det⁡(DXjTDXj), hence ∣det⁡DTj∣=rn−1Jj(y) with Jj=det⁡(DXjTDXj)>0. The inverse is z↦(∣z∣,Xj−1(z/∣z∣)), so Tj is a C1 diffeomorphism onto its open annular sector.

2.1step 1.1F3F1algebraF4

For a Borel set A⊂Sn−1, apply F3 on each sector to hj(z)=1A(z/∣z∣)χj(z/∣z∣). Its pullback times the Jacobian is the separated nonnegative function rn−11A(Xj(y))χj(Xj(y))Jj(y). Integrating this product gives C∫Uj1A(Xj)χj(Xj)Jj dy, where C=∫12rn−1dr=(2n−1)/n>0. The product integration identity follows first for simple functions of y by the defining product measure of rectangles, then by increasing simple approximation. Summing j, the partition identity shows that the volume of {z:1<∣z∣<2, z/∣z∣∈A} equals Cm(A).

3.1step 2.1F2F1algebraF4

Applying F2 to the indicator of that same annular cone gives its volume as Cσ(A). Thus Cm(A)=Cσ(A) for every Borel A, and division by the strictly positive C gives m=σ. For an orthogonal O, D(OX)TD(OX)=DXTX, while D(a+RX)TD(a+RX)=R2DXTDX. Applying F1 chartwise proves orthogonal invariance and the factor Rn−1, also for integrals by simple approximation.

4.1step 3.1F2algebra∎

Use F2 with 1B1: ∣B1∣=∫01rn−1σ(Sn−1) dr=σ(Sn−1)/n. A possible contribution at the origin is absent because the polar formula already applies to this indicator. Step 3.1 now yields the asserted chart area ∣Sn−1∣=n∣B1∣.

Source notes

Hunter §1.11, Proposition 1.45 and its preceding sphere parametrization, printed pp. 16–17 (PDF pp. 22–23). The identification with the existing cone-defined measure is proved here.

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