OAI/Geometry/RCD/Heat/KernelMeasureBounds.lean
10 declarations, 0 contain sorry, 0 declared as axioms
Continuous kernel bounds at every source pole
Bounds initially valid almost everywhere in the reference measure extend to every pole by continuity and full support. The resulting pointwise bounds may then be integrated against a singular local mass measure.
- def
OAI.RegularPointCoordinates.kernelAverageline 28Source documentation
An actual average over the testing set, in the first kernel variable.
def kernelAverage (p : ℝ → X → X → ℝ) (t : ℝ) (s : Set X) (z : X) : ℝ := …
- theorem
OAI.RegularPointCoordinates.kernelAverage_continuousline 32 - theorem
OAI.RegularPointCoordinates.continuous_bound_everywhereline 61Source documentation
Full support turns a continuous almost-everywhere inequality into an everywhere inequality. The measure used for this extension is the reference measure, not the possibly singular measure used afterwards.
theorem continuous_bound_everywhere [μ.IsOpenPosMeasure] {f g : X → ℝ} (hf : Continuous f) (hg : Continuous g) (h : ∀ᵐ z ∂μ, f z ≤ g z) : ∀ z, f z ≤ g z := by … - theorem
OAI.RegularPointCoordinates.kernelAverage_difference_everywhereline 76Source documentation
The averaged kernel difference estimate extends to every pole before it is paired with the full Bochner measure.
theorem kernelAverage_difference_everywhere [IsLocallyFiniteMeasure μ] [μ.IsOpenPosMeasure] {t : ℝ} (ht : 0 < t) {s : Set X} (hs : MeasurableSet s) (hbounded : Bornology.IsBounded s) (x : X) (B : X → ℝ) (hB : Continuous B) (h : ∀ᵐ z ∂μ, |kernelAverage μ p t s z - p t x z| ≤ B z) : ∀ z, |kernelAverage μ p t s z - p t x z| ≤ B z := … - theorem
OAI.RegularPointCoordinates.compact_weight_boundline 87 - def
OAI.RegularPointCoordinates.compactWeightline 92 - def
OAI.RegularPointCoordinates.cutoffAverageHeatMassline 102Source documentation
Average the kernel first, then integrate the cutoff average against the full mass measure.
def cutoffAverageHeatMass {E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] (M : PositiveBilinearMeasure X E) {t : ℝ} (ht : 0 < t) (s : Set X) (hs : MeasurableSet s) (hbounded : Bornology.IsBounded s) : E →L[ℝ] E := …Mentions: OAI.RegularPointCoordinates.PositiveBilinearMeasure
- theorem
OAI.RegularPointCoordinates.cutoffAverageHeatMass_energyline 112Source documentation
Fubini identifies integration of the averaged kernel with the average of the actual heat mass matrices. Compact cutoffs control the integrand even when the mass is singular.
theorem cutoffAverageHeatMass_energy {E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] (M : PositiveBilinearMeasure X E) {t : ℝ} (ht : 0 < t) (s : Set X) (hs : MeasurableSet s) (hbounded : Bornology.IsBounded s) (v : E) : ⟪v, cutoffAverageHeatMass μ hQ hp hχ hsχ M ht s hs hbounded v⟫_ℝ = (μ.real s)⁻¹ * ∫ a in s, ⟪v, cutoffHeatMass μ hQ hp hχ hsχ M ht a v⟫_ℝ ∂μ := by …Mentions: OAI.RegularPointCoordinates.PositiveBilinearMeasure, OAI.RegularPointCoordinates.cutoffAverageHeatMass, OAI.RegularPointCoordinates.cutoffHeatMass
- theorem
OAI.RegularPointCoordinates.cutoffAverageHeatMass_difference_leline 156Source documentation
The continuous all-pole extension permits the kernel difference to be integrated against singular mass, with its full quantitative bound.
theorem cutoffAverageHeatMass_difference_le {E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] [μ.IsOpenPosMeasure] (M : PositiveBilinearMeasure X E) (hχpos : ∀ z, 0 ≤ χ z) {t : ℝ} (ht : 0 < t) (s : Set X) (hs : MeasurableSet s) (hbounded : Bornology.IsBounded s) (x : X) (B : X → ℝ) (hB : Continuous B) (hbound : ∀ᵐ z ∂μ, |kernelAverage μ p t s z - p t x z| ≤ B z) (v : E) : |⟪v, (cutoffAverageHeatMass μ hQ hp hχ hsχ M ht s hs hbounded - cutoffHeatMass μ hQ hp hχ hsχ M ht x) v⟫_ℝ| ≤ ∫ z, χ z * B z ∂(M.measure v) := by …Mentions: OAI.RegularPointCoordinates.PositiveBilinearMeasure, OAI.RegularPointCoordinates.kernelAverage, OAI.RegularPointCoordinates.cutoffAverageHeatMass, OAI.RegularPointCoordinates.cutoffHeatMass
- theorem
OAI.RegularPointCoordinates.cutoffAverageHeatMass_difference_bilinear_leline 182Source documentation
The actual averaged-minus-pointwise heat mass satisfies the bilinear bound in the same full Bochner measure, including its singular part.
theorem cutoffAverageHeatMass_difference_bilinear_le {E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] [μ.IsOpenPosMeasure] (M : PositiveBilinearMeasure X E) (hχpos : ∀ z, 0 ≤ χ z) {t : ℝ} (ht : 0 < t) (s : Set X) (hs : MeasurableSet s) (hbounded : Bornology.IsBounded s) (x : X) (B : X → ℝ) (hB : Continuous B) (hbound : ∀ᵐ z ∂μ, |kernelAverage μ p t s z - p t x z| ≤ B z) (v w : E) : ⟪v, (cutoffAverageHeatMass μ hQ hp hχ hsχ M ht s hs hbounded - cutoffHeatMass μ hQ hp hχ hsχ M ht x) w⟫_ℝ ^ 2 ≤ (∫ z, χ z * B z ∂(M.measure v)) * (∫ z, χ z * B z ∂(M.measure w)) := by …Mentions: OAI.RegularPointCoordinates.PositiveBilinearMeasure, OAI.RegularPointCoordinates.kernelAverage, OAI.RegularPointCoordinates.cutoffAverageHeatMass, OAI.RegularPointCoordinates.cutoffHeatMass