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LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedaudited 2026-10-02
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The ball Poisson kernel is positive and has unit mass

Statement

Assume Countable Choice and n≥3. For every ball BR(a), interior point x and boundary point y, PR,a(x,y)>0, and the kernel has total surface mass one: ∫∂BR(a)PR,a(x,y) dSy=1.

Facts & Assumptions

Given: Countable Choice, an integer n≥3, a centre a∈Rn, a radius R>0, an interior point x∈BR(a) and a boundary point y∈∂BR(a).

[F1]

For x∈BR(a) and y∈∂BR(a) the ball Poisson kernel is PR,a(x,y)=(R2−∣x−a∣2)/(Rωn−1∣x−y∣n), the negative outward boundary-slot normal derivative of the ball Green function, and it is a continuous function of (x,y) on BR(a)×∂BR(a) (Poisson kernel of a Euclidean ball).

[F2]

Let Ω be a bounded C1 domain carrying a Dirichlet Green function whose designated correctors satisfy Hy∈C2(Ω‾); let PΩ=−∂νyGΩ. Then for every real u∈C2(Ω‾) and every x∈Ω one has u(x)=∫ΩGΩ(x,y)(−Δu(y)) dy+∫∂ΩPΩ(x,y)u(y) dS(y), both integrals absolutely finite; moreover PΩ≥0 on Ω×∂Ω and ∫∂ΩPΩ(x,y) dS(y)=1 for every x∈Ω (Green representation for classical Poisson data).

[F3]

For n≥3 the ball BR(a) carries the Dirichlet Green function G(x,z)=Φ(x−z)−(R/∣z−a∣)n−2Φ(x−z∗) (with the centre case G(x,a)=Φ(x−a)−Φ(R)), whose designated correctors all lie in C2(BR(a)‾), and whose negative outward boundary-slot normal derivative is the kernel of [F1] (Dirichlet Green function of a Euclidean ball, Poisson kernel of a Euclidean ball).

[F4]
[F5]

For n≥1 and r>0 the sphere and ball measures are ∣∂Br∣=ωn−1rn−1 and ∣Br∣=ωn−1rn/n, both finite and positive (Sphere and ball measures scale in Rn).

[F6]

Countable Choice ACω is the standing hypothesis (The Axiom of Countable Choice (ACω)).

Proof

technique · direct
1.1givenF1F2F3F4F6

Work under [F6] and let Ω:=BR(a). The hypotheses of [F2] are met: Ω is a bounded C1 domain by [F4], and by [F3] it carries a Dirichlet Green function whose designated correctors lie in C2(Ω‾); moreover the kernel PR,a of [F1] is by [F3] the negative boundary-slot normal derivative PΩ of that Green function, so the two notation systems denote the same function on Ω×∂Ω.

2.1givenstep 1.1F1F5algebra

Strict positivity. By [F1], PR,a(x,y)=(R2−∣x−a∣2)/(Rωn−1∣x−y∣n). Since x lies in the open ball, 0≤∣x−a∣<R and the numerator R2−∣x−a∣2 is positive; by [F5] both R>0 and ωn−1>0, and ∣x−y∣>0 because an interior point and a boundary point of BR(a) cannot coincide. A quotient of positive numbers is positive, so PR,a(x,y)>0.

2.2givenstep 1.1F2F3algebra

Unit mass. Apply the representation identity of [F2] on Ω=BR(a) to the constant function u≡1, which is real and lies in C2(Ω‾) with Δu=0: for every x∈Ω, 1=u(x)=∫ΩGΩ(x,y)⋅0 dy+∫∂ΩPΩ(x,y)⋅1 dS(y). Step 1.1 identifies PΩ with PR,a, and [F2] guarantees that the second integral is absolutely finite, so ∫∂BR(a)PR,a(x,y) dSy=1.

3.1step 2.1step 2.2F1F2∎

Step 2.1 gives PR,a(x,y)>0 for every interior x and boundary y, and step 2.2 gives unit total surface mass ∫∂BR(a)PR,a(x,y) dSy=1 for every x∈BR(a); this proves both assertions of the statement. The argument uses the Green representation formula rather than the ball Dirichlet theorem, so the boundary-convergence question is not presupposed.

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Sources