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TauCeti.Analysis.Sobolev.Wkp.Mollification

Interior mollification of higher weak derivatives #

For a function in W^{k+2,p}(Ω), the Fréchet derivative of the mollification of its order-k+1 weak derivative is the mollification of its order-k+2 weak derivative. The convolution uses zero extensions, but the identity holds only where the translated kernel support is contained in Ω; no regularity of the boundary is assumed.

The result supplies the successive derivative identities needed to construct smooth local approximations in the iterated weak Sobolev spaces. It uses the weak-derivative identity recorded at each graph step and the interior convolution theorem.

The classical argument is in L. C. Evans, Partial Differential Equations, §5.3.1.

theorem TauCeti.Wkp.hasFDerivAt_indicator_convolution_value {E : Type u_1} [MeasurableSpace E] [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] [BorelSpace E] {mu : MeasureTheory.Measure E} [mu.IsAddHaarMeasure] {Omega : TopologicalSpace.Opens E} {p : ENNReal} [Fact (1 ≤ p)] (u : Wkp mu Omega p 1) (rho : E → ℝ) (hrho : ContDiff ℝ (↑⊤) rho) (hrho_cpt : HasCompactSupport rho) (x : E) (hx : ∀ y ∈ tsupport rho, x - y ∈ Omega) :

The first derivative identity for the mollified Sobolev jet. The gradient stored by Wkp is converted to a linear functional using the real inner product.

@[simp]
theorem TauCeti.Wkp.fderiv_indicator_convolution_value {E : Type u_1} [MeasurableSpace E] [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] [BorelSpace E] {mu : MeasureTheory.Measure E} [mu.IsAddHaarMeasure] {Omega : TopologicalSpace.Opens E} {p : ENNReal} [Fact (1 ≤ p)] (u : Wkp mu Omega p 1) (rho : E → ℝ) (hrho : ContDiff ℝ (↑⊤) rho) (hrho_cpt : HasCompactSupport rho) (x : E) (hx : ∀ y ∈ tsupport rho, x - y ∈ Omega) :

Pointwise derivative form of hasFDerivAt_indicator_convolution_value.

theorem TauCeti.Wkp.hasFDerivAt_indicator_convolution_iteratedGradient {E : Type u_1} [MeasurableSpace E] [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] [BorelSpace E] {mu : MeasureTheory.Measure E} [mu.IsAddHaarMeasure] {Omega : TopologicalSpace.Opens E} {p : ENNReal} [Fact (1 ≤ p)] (k : ℕ) (u : Wkp mu Omega p (k + 2)) (rho : E → ℝ) (hrho : ContDiff ℝ (↑⊤) rho) (hrho_cpt : HasCompactSupport rho) (x : E) (hx : ∀ y ∈ tsupport rho, x - y ∈ Omega) :

The classical derivative of the mollified kth iterated weak-gradient field is the mollified (k+1)st field in the interior of the domain.

@[simp]
theorem TauCeti.Wkp.fderiv_indicator_convolution_iteratedGradient {E : Type u_1} [MeasurableSpace E] [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] [BorelSpace E] {mu : MeasureTheory.Measure E} [mu.IsAddHaarMeasure] {Omega : TopologicalSpace.Opens E} {p : ENNReal} [Fact (1 ≤ p)] (k : ℕ) (u : Wkp mu Omega p (k + 2)) (rho : E → ℝ) (hrho : ContDiff ℝ (↑⊤) rho) (hrho_cpt : HasCompactSupport rho) (x : E) (hx : ∀ y ∈ tsupport rho, x - y ∈ Omega) :

Pointwise derivative form of hasFDerivAt_indicator_convolution_iteratedGradient.

With a normalized smooth bump, the support condition is supplied by a closed ball contained in the domain. This version can be applied at each stage of a Sobolev jet without choosing a separate support bound for the bump.

The derivative of a normalized-bump mollification of the value of a first-order Sobolev function, at points whose bump stays in the domain.