OAI/Geometry/RCD/Heat/HarmonicBochnerHeat.lean
5 declarations, 0 contain sorry, 0 declared as axioms
The actual harmonic heat Gram and its canonical signed source
The local Bochner input, a cutoff with a weak Laplacian, and the published continuous heat kernel now give the heat Gram evolution. The source is constructed, with its full singular part and compact support retained.
- def
OAI.RegularPointCoordinates.LocalHarmonicEnergy.cutoffEnergyline 30Source documentation
The actual bounded Sobolev product representing the cutoff energy.
def cutoffEnergy (G : LocalHarmonicEnergy μ hQ U M κ p r L v) (χ : X →ᵇ ℝ) (c : SobolevSpace μ hQ) : SobolevSpace μ hQ := …Mentions: OAI.RegularPointCoordinates.LocalHarmonicEnergy, OAI.RegularPointCoordinates.SobolevSpace
- def
OAI.RegularPointCoordinates.LocalHarmonicEnergy.cutoffSourceline 35Source documentation
The canonical full signed source, not a density-only replacement.
def cutoffSource (G : LocalHarmonicEnergy μ hQ U M κ p r L v) (χ : X →ᵇ ℝ) (c : SobolevSpace μ hQ) (q : Lp ℝ 2 μ) : SignedMeasure X := …Mentions: OAI.RegularPointCoordinates.LocalHarmonicEnergy, OAI.RegularPointCoordinates.SobolevSpace
- theorem
OAI.RegularPointCoordinates.LocalHarmonicEnergy.cutoffEnergy_coeline 41Source documentation
This product has exactly the required cutoff Gram representative.
theorem cutoffEnergy_coe (G : LocalHarmonicEnergy μ hQ U M κ p r L v) (χ : X →ᵇ ℝ) (hχΩ : tsupport (χ : X → ℝ) ⊆ ball p (2 * r)) (c : SobolevSpace μ hQ) (hc : SobolevSpace.toLp μ hQ c =ᵐ[μ] χ) : SobolevSpace.toLp μ hQ (G.cutoffEnergy μ hQ χ c) =ᵐ[μ] fun x => χ x * (SobolevSpace.minimalSlope μ hQ (U v) x) ^ 2 := by …Mentions: OAI.RegularPointCoordinates.LocalHarmonicEnergy, OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.SobolevSpace.minimalSlope
- theorem
OAI.RegularPointCoordinates.LocalHarmonicEnergy.cutoffEnergy_laplacianline 63Source documentation
The global measure equation is derived from the local Bochner equation.
theorem cutoffEnergy_laplacian (G : LocalHarmonicEnergy μ hQ U M κ p r L v) (χ : X →ᵇ ℝ) (hχs : HasCompactSupport (χ : X → ℝ)) (hχΩ : tsupport (χ : X → ℝ) ⊆ ball p (2 * r)) (c : SobolevSpace μ hQ) (hc : SobolevSpace.toLp μ hQ c =ᵐ[μ] χ) (q : Lp ℝ 2 μ) (hq : IsWeakLaplacian μ hQ c q) : IsMeasureLaplacian μ hQ (G.cutoffEnergy μ hQ χ c) (G.cutoffSource μ hQ χ c q) := …Mentions: OAI.RegularPointCoordinates.LocalHarmonicEnergy, OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.IsWeakLaplacian, OAI.RegularPointCoordinates.IsMeasureLaplacian
- theorem
OAI.RegularPointCoordinates.LocalHarmonicEnergy.heatGram_hasDerivAtline 75Source documentation
Full-source evolution of the actual harmonic heat Gram. Compact support hypotheses concern only the cutoff and its weak Laplacian.
theorem heatGram_hasDerivAt (G : LocalHarmonicEnergy μ hQ U M κ p r L v) (χ : X →ᵇ ℝ) (hχs : HasCompactSupport (χ : X → ℝ)) (hχΩ : tsupport (χ : X → ℝ) ⊆ ball p (2 * r)) (c : SobolevSpace μ hQ) (hc : SobolevSpace.toLp μ hQ c =ᵐ[μ] χ) (q : Lp ℝ 2 μ) (hq : IsWeakLaplacian μ hQ c q) (a : X) {R : ℝ} (hR : 0 < R) (hχR : ∀ x ∉ closedBall a R, χ x = 0) (hqR : ∀ᵐ x ∂μ, x ∉ closedBall a R → q x = 0) {t : ℝ} (ht : 0 < t) (x : X) (lambda : ℝ) : HasDerivAt (fun s => ⟪v, cutoffHeatGramAt μ hQ hk χ.continuous hχs U s x lambda v⟫_ℝ) ((∫ᵛ z, k t x z ∂<•(G.cutoffSource μ hQ χ c q)) + lambda * ‖v‖ ^ 2) t := by …Mentions: OAI.RegularPointCoordinates.LocalHarmonicEnergy, OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.IsWeakLaplacian, OAI.RegularPointCoordinates.cutoffHeatGramAt