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Green representation outside a ball for compactly supported C² functions

Proved
HunterPDE.Newtonian.punctured_green_identity

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

green-identitiesintegrationnewtonian-potential

Let n≥2n\ge2n≥2, f∈Cc2(Rn)f\in C_c^2(\mathbb R^n)f∈Cc2​(Rn), x∈Rnx\in\mathbb R^nx∈Rn, r>0r>0r>0, and let vvv be any unit vector. Write Af(x,r)A_f(x,r)Af​(x,r) for the normalized surface average of fff on ∂Br(x)\partial B_r(x)∂Br​(x). Then

∫Rn∖Br(x)Γn(x−y)Δf(y) dy=−Γn(rv)∫Br(x)Δf(y) dy−Af(x,r).\int_{\mathbb R^n\setminus B_r(x)}\Gamma_n(x-y)\Delta f(y)\,dy =-\Gamma_n(rv)\int_{B_r(x)}\Delta f(y)\,dy-A_f(x,r).∫Rn∖Br​(x)​Γn​(x−y)Δf(y)dy=−Γn​(rv)∫Br​(x)​Δf(y)dy−Af​(x,r).

This is the finite-radius Green representation in Hunter's Eq. (2.20), with the outward derivative flux of fff expressed as a ball integral of its Laplacian. The kernel is radial, so the choice of unit vector has no effect. This formula isolates the integration-by-parts argument before the singular radius tends to zero.

Preamble
import Definitions.Def_HunterPDE_Newtonian_FundamentalSolution
import Definitions.Def_HunterPDE_Harmonic_MeanValue
import Mathlib.Analysis.InnerProductSpace.Laplacian

open MeasureTheory Filter Set Topology
open scoped ContDiff
open Laplacian
open HunterPDE.Newtonian HunterPDE.Harmonic
Formal statement
theorem HunterPDE.Newtonian.punctured_green_identity (n : ℕ) (hn : 2 ≤ n)
    (f : EuclideanSpace ℝ (Fin n) → ℝ) (hf : ContDiff ℝ 2 f) (hfc : HasCompactSupport f)
    (x v : EuclideanSpace ℝ (Fin n)) (hv : ‖v‖ = 1) (r : ℝ) (hr : 0 < r) :
    (∫ y in (Metric.ball x r)ᶜ, fundamentalSolution n (x - y) * (Δ f) y) =
      -fundamentalSolution n (r • v) * (∫ y in Metric.ball x r, (Δ f) y) -
        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 pp. 33–36: Eq. (2.12), local integrability in §2.6.1, Eq. (2.19)–(2.23); Green identity Eq. (2.11), printed p. 32. The ball-integral form of the boundary flux uses the divergence theorem, Theorem 1.46, printed p. 17.

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