OAI/Geometry/RCD/Harmonic/RadialLinearRepresentatives.lean
2 declarations, 0 contain sorry, 0 declared as axioms
Finite radial families preserve all constant covectors
- theorem
OAI.RegularPointCoordinates.localRadialDerivative_columnline 18Source documentation
Once the basis radial derivatives have Sobolev representatives, their linear combinations are the radial derivatives of every coordinate covector.
theorem localRadialDerivative_column {n : ℕ} (Ω : Set X) (f : SobolevSpace μ hQ) {B : ℝ} (hf : ∀ᵐ x ∂μ.restrict Ω, localGamma μ hQ f f x ≤ B) (u g : Fin n → SobolevSpace μ hQ) (hg : ∀ j, SobolevSpace.toLp μ hQ (g j) =ᵐ[μ.restrict Ω] localGamma μ hQ f (u j)) (b : Euclidean n) : localRadialDerivative μ hQ Ω f hf (sobolevColumnMap μ hQ u b) = SobolevSpace.restrictLp μ hQ Ω (sobolevColumnMap μ hQ g b) := by …Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.localGamma, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.Euclidean, OAI.RegularPointCoordinates.localRadialDerivative, OAI.RegularPointCoordinates.sobolevColumnMap, OAI.RegularPointCoordinates.SobolevSpace.restrictLp
- theorem
OAI.RegularPointCoordinates.localRadialDerivative_constantline 32Source documentation
The derivative kills every compactly extended local constant.
theorem localRadialDerivative_constant (Ω : Set X) (f q : SobolevSpace μ hQ) {B : ℝ} (hf : ∀ᵐ x ∂μ.restrict Ω, localGamma μ hQ f f x ≤ B) (c : ℝ) (hq : SobolevSpace.toLp μ hQ q =ᵐ[μ.restrict Ω] fun _ => c) : localRadialDerivative μ hQ Ω f hf q = 0 := by …Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.localGamma, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.localRadialDerivative