OAI/Geometry/RCD/Heat/HeatMeasureEvolution.lean
3 declarations, 0 contain sorry, 0 declared as axioms
The heat identity for a full compactly supported signed Laplacian
The distributional source is paired with continuous positive-time kernel rows. Locality supplies the compact test, and the actual L2 heat equation supplies the derivative. This proves the positive-endpoint measure-source identity without assuming absolute continuity of the source.
- theorem
OAI.RegularPointCoordinates.kernelHeat_hasDerivAtline 29Source documentation
Pointwise time differentiation of the continuous representative of heat flow from actual Sobolev data.
theorem kernelHeat_hasDerivAt (u : SobolevSpace μ hQ) {t : ℝ} (ht : 0 < t) (x : X) : HasDerivAt (fun s => kernelHeat μ hQ hp s (SobolevSpace.toLp μ hQ u) x) (-energyForm μ hQ u (heatKernelSobolev μ hQ hp t ht x)) t := by …Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.kernelHeat, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.energyForm, OAI.RegularPointCoordinates.heatKernelSobolev
- theorem
OAI.RegularPointCoordinates.IsMeasureLaplacian.kernelHeat_hasDerivAtline 54Source documentation
The pointwise derivative against the full signed source.
theorem IsMeasureLaplacian.kernelHeat_hasDerivAt {u : SobolevSpace μ hQ} {ν : SignedMeasure X} (hν : IsMeasureLaplacian μ hQ u ν) (c : X) {R : ℝ} (hR : 0 < R) (hu : ∀ᵐ x ∂μ, R < dist c x → SobolevSpace.toLp μ hQ u x = 0) (hsν : ν.variation (Metric.closedBall c R)ᶜ = 0) {t : ℝ} (ht : 0 < t) (x : X) : HasDerivAt (fun s => kernelHeat μ hQ hp s (SobolevSpace.toLp μ hQ u) x) (∫ᵛ z, p t x z ∂<•ν) t := by …Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.IsMeasureLaplacian, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.kernelHeat
- theorem
OAI.RegularPointCoordinates.IsMeasureLaplacian.kernelHeat_sub_eq_integralline 68Source documentation
The manuscript's positive-endpoint semigroup identity for compact measure sources, using continuous representatives and the full measure.
theorem IsMeasureLaplacian.kernelHeat_sub_eq_integral {u : SobolevSpace μ hQ} {ν : SignedMeasure X} (hν : IsMeasureLaplacian μ hQ u ν) (c : X) {R : ℝ} (hR : 0 < R) (hu : ∀ᵐ x ∂μ, R < dist c x → SobolevSpace.toLp μ hQ u x = 0) (hsν : ν.variation (Metric.closedBall c R)ᶜ = 0) {s t : ℝ} (hs : 0 < s) (hst : s ≤ t) (x : X) : kernelHeat μ hQ hp t (SobolevSpace.toLp μ hQ u) x - kernelHeat μ hQ hp s (SobolevSpace.toLp μ hQ u) x = ∫ r in s..t, (∫ᵛ z, p r x z ∂<•ν) := by …Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.IsMeasureLaplacian, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.kernelHeat