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Mixed Green identity on a spherical annulus

Proved
MeasureTheory.mixed_green_identity_annulus

by Mazecto · Oct 10, 2026 · Mathlib 0df444a (Lean v4.33.1)

divergence-theoremintegration-by-partsmultivariable-calculus

Let n≥1n\ge1n≥1, let K:Rn→RK:\mathbb R^n\to\mathbb RK:Rn→R be smooth away from the origin, and let g:Rn→Rg:\mathbb R^n\to\mathbb Rg:Rn→R be C2C^2C2. Fix x∈Rnx\in\mathbb R^nx∈Rn, coordinate indices i,ji,ji,j, and 0<r<R0<r<R0<r<R. Put

A=BR(x)∖B‾r(x),A=B_R(x)\setminus\overline B_r(x),A=BR​(x)∖Br​(x),

and define the surface expression

Hs(K,g)=∫Sn−1[K(−sω)∂jg(x+sω)ωi+∂iK(−sω)g(x+sω)ωj]dS(ω).H_s(K,g)=\int_{S^{n-1}}\left[K(-s\omega)\partial_jg(x+s\omega)\omega_i+\partial_iK(-s\omega)g(x+s\omega)\omega_j\right]dS(\omega).Hs​(K,g)=∫Sn−1​[K(−sω)∂j​g(x+sω)ωi​+∂i​K(−sω)g(x+sω)ωj​]dS(ω).

Then

∫A∂ijK(x−y)g(y) dy=∫AK(x−y)∂ijg(y) dy−Rn−1HR(K,g)+rn−1Hr(K,g).\int_A\partial_{ij}K(x-y)g(y)\,dy=\int_AK(x-y)\partial_{ij}g(y)\,dy-R^{n-1}H_R(K,g)+r^{n-1}H_r(K,g).∫A​∂ij​K(x−y)g(y)dy=∫A​K(x−y)∂ij​g(y)dy−Rn−1HR​(K,g)+rn−1Hr​(K,g).

The outer normal of the annulus is ω\omegaω on the outer sphere and −ω-\omega−ω on the inner sphere. The formula follows by integrating the mixed Green differential identity twice; smoothness permits the interchange of mixed derivatives. No compact support, radiality, harmonicity, or growth assumption is required. All evaluation points of the kernel on the closed annulus avoid the origin. The derivatives are coordinate Fréchet derivatives, and dSdSdS is the surface measure induced by Lebesgue volume.

Preamble
import Definitions.Def_HunterPDE_Newtonian_PartialDeriv
import Mathlib.Analysis.Calculus.ContDiff.Basic
import Mathlib.MeasureTheory.Integral.Bochner.Set
import Mathlib.MeasureTheory.Constructions.HaarToSphere
import Mathlib.MeasureTheory.Measure.Haar.InnerProductSpace

open MeasureTheory HunterPDE.Newtonian
open scoped ContDiff
Formal statement
theorem MeasureTheory.mixed_green_identity_annulus
    (n : ℕ) (hn : 0 < n) (K : EuclideanSpace ℝ (Fin n) → ℝ)
    (hK : ContDiffOn ℝ ∞ K {0}ᶜ)
    (g : EuclideanSpace ℝ (Fin n) → ℝ) (hg : ContDiff ℝ 2 g)
    (x : EuclideanSpace ℝ (Fin n)) (R r : ℝ) (hR : 0 < R)
    (hr : 0 < r) (hrR : r < R) (i j : Fin n) :
    (∫ y in Metric.ball x R \ Metric.closedBall x r,
      secondPartial K i j (x - y) * g y) =
    (∫ y in Metric.ball x R \ Metric.closedBall x r,
      K (x - y) * secondPartial g i j y)
    - R ^ (n - 1) *
      (∫ (w : Metric.sphere (0 : EuclideanSpace ℝ (Fin n)) 1),
        K (-(R • w.1)) * partialDeriv g j (x + R • w.1) * w.1 i
        + partialDeriv K i (-(R • w.1)) * g (x + R • w.1) * w.1 j
        ∂volume.toSphere)
    + r ^ (n - 1) *
      (∫ (w : Metric.sphere (0 : EuclideanSpace ℝ (Fin n)) 1),
        K (-(r • w.1)) * partialDeriv g j (x + r • w.1) * w.1 i
        + partialDeriv K i (-(r • w.1)) * g (x + r • w.1) * w.1 j
        ∂volume.toSphere) := by sorry
Source
Hunter, Notes on Partial Differential Equations, revised 6/18/2014, https://www.math.ucdavis.edu/~hunter/pdes/ch2.pdf, printed pp. 37–38, differential identity preceding Eq. (2.27) and Green integration in (2.27). General smooth-kernel formulation on a spherical annulus; boundary surface measure is parametrized by the unit sphere.

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