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Exterior Green formula for a kernel with Coulomb radial gradient

Proved
MeasureTheory.exterior_green_of_coulomb_gradient

by Mazecto · Oct 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

green-identitiesintegrationpotential-theory

Let n≥2n\ge2n≥2, and let KKK be smooth on Rn∖{0}\mathbb R^n\setminus\{0\}Rn∖{0}. Suppose that a real constant ccc satisfies

∂iK(z)=c ∣z∣1−nzi∣z∣(z≠0, 1≤i≤n).\partial_iK(z)=c\,|z|^{1-n}\frac{z_i}{|z|}\qquad(z\ne0,\ 1\le i\le n).∂i​K(z)=c∣z∣1−n∣z∣zi​​(z=0, 1≤i≤n).

Let f∈Cc2(Rn)f\in C_c^2(\mathbb R^n)f∈Cc2​(Rn), x∈Rnx\in\mathbb R^nx∈Rn, and r>0r>0r>0. Suppose K(z)=κK(z)=\kappaK(z)=κ whenever ∣z∣=r|z|=r∣z∣=r. Write αn\alpha_nαn​ for the volume of the unit ball and Af(x,r)A_f(x,r)Af​(x,r) for the normalized surface average of fff. Then

∫Rn∖Br(x)K(x−y)Δf(y) dy=−κ∫Br(x)Δf(y) dy+nαnc Af(x,r).\int_{\mathbb R^n\setminus B_r(x)}K(x-y)\Delta f(y)\,dy=-\kappa\int_{B_r(x)}\Delta f(y)\,dy+n\alpha_n c\,A_f(x,r).∫Rn∖Br​(x)​K(x−y)Δf(y)dy=−κ∫Br​(x)​Δf(y)dy+nαn​cAf​(x,r).

This is the compact-support exterior specialization of Green's second identity, with the derivative flux expressed as a ball Laplacian integral. It applies to arbitrary scalar multiples and additive constants of the logarithmic and Newtonian kernels, and isolates the integration-by-parts step from singular-radius limits.

Preamble
import Definitions.Def_HunterPDE_Harmonic_MeanValue
import Mathlib.Analysis.InnerProductSpace.Laplacian
import Mathlib.Analysis.Calculus.ContDiff.Basic

open MeasureTheory Set
open scoped ContDiff
open Laplacian
open HunterPDE.Harmonic

Formal statement
theorem MeasureTheory.exterior_green_of_coulomb_gradient
    (n : ℕ) (hn : 2 ≤ n) (K : EuclideanSpace ℝ (Fin n) → ℝ)
    (hK : ContDiffOn ℝ ∞ K {0}ᶜ) (c : ℝ)
    (hDK : ∀ z : EuclideanSpace ℝ (Fin n), z ≠ 0 → ∀ i : Fin n,
      fderiv ℝ K z (EuclideanSpace.single i 1) =
        c * (1 / ‖z‖ ^ (n - 1)) * (z i / ‖z‖))
    (f : EuclideanSpace ℝ (Fin n) → ℝ) (hf : ContDiff ℝ 2 f)
    (hfc : HasCompactSupport f) (x : EuclideanSpace ℝ (Fin n))
    (r : ℝ) (hr : 0 < r) (κ : ℝ)
    (hκ : ∀ z : EuclideanSpace ℝ (Fin n), ‖z‖ = r → K z = κ) :
    (∫ y in (Metric.ball x r)ᶜ, K (x - y) * (Δ f) y) =
      -κ * (∫ y in Metric.ball x r, (Δ f) y) +
        ((n : ℝ) * volume.real (Metric.ball (0 : EuclideanSpace ℝ (Fin n)) 1) * c) *
          sphereAverage f x r := by sorry
Source
John K. Hunter, Notes on Partial Differential Equations, revised 6/18/2014, https://www.math.ucdavis.edu/~hunter/pdes/pde_notes.pdf, printed p. 32, Eq. (2.11); pp. 33–36, Eqs. (2.14), (2.15), (2.20); p. 17, Theorem 1.46. Generalization allowing an arbitrary gradient coefficient and boundary constant.

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