Alphabeta Math
LemmaStatement: AI-adaptedProof: AI-generatedPipeline-generatedprecheck passjudge pass (gpt-6.1-sol)audited 2026-10-08
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Weighted monomial integrals and monomial norms for the disc, ball and polydisc

Facts & Assumptions

Given: An integer m≥1, the Axiom of Countable Choice ACω, and a multi-index α=(α0,…,αm−1)∈Nm. Write α!:=∏j<mαj!, ∣α∣:=∑j<mαj, and zα:=∏j<mzjαj using the conventions of Ck maps and multi-index derivative notation in Euclidean space and Integer powers in the complex field.

For d≥1, β∈Nd and t∈N, write Id(β,t):=∫Bd∣zβ∣2(1−∣z∣2)t dλ2d(z).

[A1]

The only choice principle assumed is ACω (The Axiom of Countable Choice (ACω)). It is required by the polar-coordinate, chart/polar surface, sigma-finiteness and product-Lebesgue suppliers below; no full Axiom of Choice or arbitrary-index selection is used.

[F1]

The complex-real identification and Euclidean norm are those of Complex m-space and its real coordinate dictionary, and the open unit ball Bm and open unit polydisc Dm are those of Balls, polydiscs and the distinguished boundary in Cm.

[F2]

For every nonnegative Borel function on Rn, polar coordinates give ∫f dλn=∫0∞∫Sn−1f(rω)rn−1 dσ(ω) dr (The polar surface set function on the unit sphere, Polar coordinates decompose Lebesgue measure into r^{n-1} dr d sigma).

[F3]

On each angular chart X(θ)=(cos⁡θ,sin⁡θ) of S1, the derivative has norm 1, so the surface density is 1; summing a partition of unity over one full turn gives chart surface measure ∫02π1 dθ=2π. The chart surface measure equals the polar measure σ (Surface integration on compact C1 hypersurfaces, Agreement with the existing polar sphere measure).

[F4]

For p,q>0, the Euler Beta integral is B(p,q)=∫01tp−1(1−t)q−1 dt and converges (Euler's real Beta integral, Euler's Beta integral converges exactly for two positive parameters); change of variables is valid on the improper interval after compact truncation (Change of variable in an improper integral).

[F5]

The Beta-Gamma identity is B(p,q)=Γ(p)Γ(q)/Γ(p+q), and Γ(n+1)=n! for every n∈N (The real Beta--Gamma identity, Γ(n+1)=n! for every natural number n, The factorial n! and the falling factorial nk‾, defined by recursion in N).

[F6]

Nonnegative product-measurable functions satisfy Tonelli's iterated-integral identity on sigma-finite measure spaces; under ACω, product Lebesgue measure agrees with Euclidean Lebesgue measure on Borel sets, and equality of these measures gives equality of nonnegative integrals by simple approximation and monotone convergence (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product, The Borel product of R^m and R^n is the Borel sigma-algebra of R^{m+n}, On Borel subsets of R^{m+n}, the product lambda_m times lambda_n agrees with lambda_{m+n}, Lebesgue measure is sigma-finite, and every metrically bounded subset of Rn has finite outer measure, Every nonnegative measurable function admits an explicit increasing sequence of simple approximations, Monotone convergence for the integral).

[F7]

In real coordinates the displayed integrands are nonnegative polynomials times indicators of open balls or polydiscs. Finite sums and products of coordinate polynomials are continuous by the Ck algebra theorem; the preimage criterion makes continuous maps Borel measurable, and products of measurable functions remain measurable (Ck Euclidean maps and diffeomorphisms, Ck Euclidean maps are closed under componentwise algebra and composition, The Borel sigma-algebra of a topological space, A measurable function between measurable spaces, A continuous map has Borel preimages of Borel sets, Arithmetic and lattice operations preserve measurability whenever they are defined, Balls, polydiscs and the distinguished boundary in Cm).

[F8]
[F10]

Induction on the positive integer dimension is valid (The principle of mathematical induction).

[F9]

Multi-indices, their factorials and lengths, and complex nonnegative integer powers have the conventions used in the statement (Ck maps and multi-index derivative notation in Euclidean space, The factorial n! and the falling factorial nk‾, defined by recursion in N, Integer powers in the complex field).

Statement

Assume ACω (The Axiom of Countable Choice (ACω)). Let m≥1, and let λ2m be Lebesgue measure under Cm≅R2m. For every α∈Nm and every integer s≥0,

∫Bm∣zα∣2(1−∣z∣2)s dλ2m(z)=πmα! s!(m+s+∣α∣)!.

In particular,

∫Bm∣zα∣2 dλ2m(z)=πmα!(m+∣α∣)!,λ2m(Bm)=πmm!.

For the unit polydisc and the one-dimensional disc,

∫Dm∣zα∣2 dλ2m(z)=πm∏j<m(αj+1),λ2m(Dm)=πm,

and for every integer k≥0,

∫D∣z∣2k dλ2(z)=πk+1.

Proof

technique · direct, using a one-variable polar integral and induction by slicing the ball

Given: m≥1, ACω, and α∈Nm; the indices in zα use the zero-based convention in [F1] and [F9].

1.1A1F2F3F7given

For integers k,s≥0 and ρ>0, let Jk,s(ρ):=∫∣w∣<ρ∣w∣2k(ρ2−∣w∣2)s dλ2(w). The integrand extended by zero outside the disc is nonnegative Borel by [F7]. By [F2] and [F3], Jk,s(ρ)=2π∫0ρr2k+1(ρ2−r2)s dr.

2.1F4step 1.1givenalgebra

The substitution t=(r/ρ)2 is increasing from (0,ρ) onto (0,1) and has r dr=ρ2dt/2. Thus [F4] gives Jk,s(ρ)=πρ2(k+s+1)B(k+1,s+1).

3.1F5step 2.1givenalgebra

By [F5], B(k+1,s+1)=Γ(k+1)Γ(s+1)/Γ(k+s+2)=k!s!/(k+s+1)!. Hence Jk,s(ρ)=πρ2(k+s+1)k!s!/(k+s+1)!.

4.1F1F9step 3.1given

In dimension m=1, writing α=(k) and taking ρ=1 in step 3.1 gives I1((k),s)=πk!s!/(k+s+1)!, the asserted formula.

4.2A1F1F6F7F8F9step 3.1given

Fix m≥2 and assume the ball formula in dimension m−1 for all multi-indices and nonnegative integer weights. Write α=(α′,k) and slice Bm⊆Cm−1×C at z′∈Bm−1; its last-coordinate slice is ∣w∣<ρ(z′), where ρ(z′)=(1−∣z′∣2)1/2>0 by [F8]. For z′∉Bm−1 the slice is empty. By Tonelli, product-Lebesgue agreement, and step 3.1, Im(α,s)=πk!s!(k+s+1)!Im−1(α′,k+s+1).

4.3A1F1F6F7F9step 3.1given

The unit polydisc is the product of m unit discs and ∣zα∣2=∏j<m∣zj∣2αj. Repeated application of Tonelli and product-Lebesgue agreement, followed by step 3.1 with s=0 and ρ=1 in each coordinate, gives ∫Dm∣zα∣2 dλ2m=∏j<mπ/(αj+1)=πm/∏j<m(αj+1).

5.1F9F10step 4.1step 4.2givenalgebradischarge-induction

Substitution of the induction hypothesis into step 4.2 gives Im(α,s)=πk!s!(k+s+1)!⋅πm−1α′!(k+s+1)!(m+s+k+∣α′∣)!=πmα!s!(m+s+∣α∣)!, since α!=α′!k! and ∣α∣=∣α′∣+k. The base case step 4.1 and this induction step prove the weighted ball formula in every positive dimension by [F10].

6.1F9step 5.1step 4.3given∎

Setting s=0 in the ball formula gives its unweighted monomial integral; setting also α=0 gives λ2m(Bm)=πm/m!. Setting α=0 in step 4.3 gives λ2m(Dm)=πm, and the case m=1, s=0, α=(k) in the ball formula gives the stated disc integral.

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