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LeanPool.CaffarelliKohnNirenberg.Pressure.LeibnizLaplacian

The Leibniz rule for the spatial Laplacian, in weak form #

The paper's identity eq:leibniz-lap, Δ(η T) = η Δ T + 2 ∂_j η ∂_j T + T Δ η, is stated there for a scalar distribution T and a smooth η. This file proves the underlying pointwise second-order product rule for smooth functions on Vec3 := Fin 3 → ℝ, and then integrates it against a locally integrable weight to obtain the weak (test-function) form used in the paper.

Spatial partial derivatives are ordinary partial derivatives, expressed as the Fréchet derivative applied to a coordinate basis vector, matching the convention of CKN.spatialPartial.

Spatial partial derivatives and their product rules #

The ith spatial partial derivative ∂_i f, as the Fréchet derivative applied to the ith coordinate basis vector.

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    The spatial Laplacian Δ f = ∑_i ∂_i ∂_i f.

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      The Euclidean gradient pairing ∇f · ∇g = ∑_i ∂_i f ∂_i g.

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        The mixed second derivative ∂_i ∂_j f.

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          theorem CKN.spatialSecondDeriv_mul_smooth {η φ : Foundation.Parabolic.Vec3 → ℝ} (hη : ContDiff ℝ (↑⊤) η) (hφ : ContDiff ℝ (↑⊤) φ) (i j : Fin 3) (x : Foundation.Parabolic.Vec3) :
          mixedSecond (fun (y : Foundation.Parabolic.Vec3) => η y * φ y) i j x = mixedSecond η i j x * φ x + spatialDeriv η j x * spatialDeriv φ i x + spatialDeriv η i x * spatialDeriv φ j x + η x * mixedSecond φ i j x

          The pointwise second-order product rule ∂_i ∂_j (η φ) of eq:leibniz-lap and eq:commute.

          theorem CKN.spatialLaplacian_mul_smooth {η φ : Foundation.Parabolic.Vec3 → ℝ} (hη : ContDiff ℝ (↑⊤) η) (hφ : ContDiff ℝ (↑⊤) φ) :
          (spatialLaplacian fun (x : Foundation.Parabolic.Vec3) => η x * φ x) = fun (x : Foundation.Parabolic.Vec3) => η x * spatialLaplacian φ x + 2 * spatialGradDot η φ x + φ x * spatialLaplacian η x

          The pointwise Leibniz rule eq:leibniz-lap for the spatial Laplacian: Δ(η φ) = η Δφ + 2 ∇η · ∇φ + φ Δη.