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LeanPool.ViscositySolutionTheory.ViscositySolns.Applications.Laplace.Weyl.LaplacianInvariance

Invariance of the Laplacian and radial Laplacians (ported from TauCeti) #

For a finite-dimensional real inner product space E and any f : E → F:

The invariance statements need no differentiability hypothesis on f.

Provenance #

Pool port: imports relocated under LeanPool.ViscositySolutionTheory; original mathematical namespaces and copyright retained; checked with Lean/Mathlib v4.34.0.

theorem ViscositySolns.Analysis.iteratedFDeriv_comp_linearIsometryEquiv_apply {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] {E' : Type u_2} [NormedAddCommGroup E'] [InnerProductSpace ℝ E'] {F : Type u_3} [NormedAddCommGroup F] [NormedSpace ℝ F] (l : E ≃ₗᵢ[ℝ] E') (f : E' → F) (i : ℕ) (x : E) (m : Fin i → E) :
(iteratedFDeriv ℝ i (f ∘ ⇑l) x) m = (iteratedFDeriv ℝ i f (l x)) fun (j : Fin i) => l (m j)

The iterated derivative transforms under a linear isometry equivalence on the right by pulling the directions through the isometry.

Invariance of the Laplacian under isometries. Δ (f ∘ l) = (Δ f) ∘ l for a linear isometry equivalence l. No differentiability hypothesis is needed.

theorem ViscositySolns.Analysis.laplacian_comp_add_right {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] {F : Type u_3} [NormedAddCommGroup F] [NormedSpace ℝ F] (f : E → F) (a : E) :
(Laplacian.laplacian fun (y : E) => f (y + a)) = fun (y : E) => Laplacian.laplacian f (y + a)

Translation invariance of the Laplacian. No differentiability hypothesis is needed.

theorem ContDiff.laplacian_comp_norm_sq {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] {ρ : ℝ → ℝ} (hρ : ContDiff ℝ 2 ρ) (x : E) :
Laplacian.laplacian (fun (y : E) => ρ (‖y‖ ^ 2)) x = 4 * ‖x‖ ^ 2 * deriv (deriv ρ) (‖x‖ ^ 2) + 2 * ↑(Module.finrank ℝ E) * deriv ρ (‖x‖ ^ 2)

The Laplacian of a radial function. For a C² function ρ : ℝ → ℝ, the Laplacian of x ↦ ρ (‖x‖ ^ 2) is 4 ‖x‖² ρ'' (‖x‖²) + 2 (dim E) ρ' (‖x‖²).

The Laplacian vanishes wherever the function vanishes identically: Δ is local.