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Atlas.DifferentialAnalysis.code.PseudoDiffComposition

A smooth -valued function on ℝⁿ whose iterated derivatives of every order decay to zero at infinity (i.e. tend to 0 along the cocompact filter).

Instances For
    @[implicit_reducible]

    Treat SmoothZeroAtInfty n as a FunLike so that an element can be applied like a function.

    theorem PoissonEquation.SmoothZeroAtInfty.ext {n : } {f g : SmoothZeroAtInfty n} (h : ∀ (x : EuclideanSpace (Fin n)), f x = g x) :
    f = g

    Pointwise extensionality for SmoothZeroAtInfty.

    An element of SmoothZeroAtInfty n is C^∞ smooth.

    The m-th iterated derivative norm of f : SmoothZeroAtInfty n tends to 0 at infinity.

    IsLaplacianOf n f g says that g = -Δ f pointwise, where Δ is the standard Laplacian on ℝⁿ defined via the iterated Fréchet derivative.

    Instances For
      theorem PoissonEquation.harmonic_fderiv_norm_le_div {n : } (hn : 1 n) (u : EuclideanSpace (Fin n)) (hsmooth : ContDiff (↑) u) (hharm : IsLaplacianOf n u 0) (C : ) (hC : 0 C) (hbd : ∀ (x : EuclideanSpace (Fin n)), u x C) (R : ) (hR : 0 < R) (a : EuclideanSpace (Fin n)) :
      fderiv u a n * C / R

      Gradient estimate (mean value inequality) for a bounded harmonic function: ‖∇u(a)‖ ≤ n · C / R for any radius R > 0.

      theorem PoissonEquation.bounded_harmonic_fderiv_eq_zero {n : } (hn : 1 n) (u : EuclideanSpace (Fin n)) (hsmooth : ContDiff (↑) u) (hharm : IsLaplacianOf n u 0) (hbd : ∃ (C : ), ∀ (x : EuclideanSpace (Fin n)), u x C) (x : EuclideanSpace (Fin n)) :
      fderiv u x = 0

      Liouville-type derivative vanishing: a bounded harmonic function has zero Fréchet derivative everywhere.

      theorem PoissonEquation.bounded_harmonic_is_constant {n : } (hn : 1 n) (u : EuclideanSpace (Fin n)) (hsmooth : ContDiff (↑) u) (hharm : IsLaplacianOf n u 0) (hbd : ∃ (C : ), ∀ (x : EuclideanSpace (Fin n)), u x C) :
      ∃ (c : ), u = Function.const (EuclideanSpace (Fin n)) c

      Liouville's theorem: a bounded harmonic function on ℝⁿ is constant.

      theorem PoissonEquation.laplacianOp_smooth_eq_classical {n : } (hn : 3 n) (u : SmoothZeroAtInfty n) (u_td : TemperedDistribution (EuclideanSpace (Fin n)) ) (hu_td : ∀ (φ : SchwartzMap (EuclideanSpace (Fin n)) ), u_td φ = (x : EuclideanSpace (Fin n)), φ x u x) (φ : SchwartzMap (EuclideanSpace (Fin n)) ) :
      (DifferentialOperators.laplacianOp u_td) φ = (x : EuclideanSpace (Fin n)), φ x -j : Fin n, (iteratedFDeriv 2 (⇑u) x) fun (x : Fin 2) => EuclideanSpace.single j 1

      Integration by parts: for a smooth, decaying u representing a tempered distribution u_td, the distributional Laplacian acts as the pointwise classical Laplacian against test functions.

      theorem PoissonEquation.schwartz_determines_continuous {n : } (hn : 3 n) (u : SmoothZeroAtInfty n) (f : SchwartzMap (EuclideanSpace (Fin n)) ) (h : ∀ (φ : SchwartzMap (EuclideanSpace (Fin n)) ), ( (x : EuclideanSpace (Fin n)), φ x -j : Fin n, (iteratedFDeriv 2 (⇑u) x) fun (x : Fin 2) => EuclideanSpace.single j 1) = (x : EuclideanSpace (Fin n)), φ x f x) (x : EuclideanSpace (Fin n)) :
      f x = -j : Fin n, (iteratedFDeriv 2 (⇑u) x) fun (x : Fin 2) => EuclideanSpace.single j 1

      Schwartz testing determines continuous functions pointwise: if two continuous functions integrate identically against every Schwartz test, they coincide.

      The distributional Laplacian of u agrees with the pointwise Laplacian when both are defined and u is smooth and decaying.

      Existence of a smooth, decaying Laplacian inverse for a Schwartz right-hand side f in dimension n ≥ 3.

      theorem PoissonEquation.laplacian_injective {n : } (hn : 3 n) (u₁ u₂ : SmoothZeroAtInfty n) (f : EuclideanSpace (Fin n)) (h₁ : IsLaplacianOf n (⇑u₁) f) (h₂ : IsLaplacianOf n (⇑u₂) f) :
      u₁ = u₂

      Injectivity of the Laplacian on SmoothZeroAtInfty n: two decaying solutions of -Δuᵢ = f agree.