OAI/Geometry/RCD/Heat/ActualHeatMass.lean
8 declarations, 0 contain sorry, 0 declared as axioms
Heat averages of full local mass measures
The weight is the same actual heat kernel and compact cutoff used in the Gram matrices. The mass can have a singular part and is identified locally with the Bochner measure.
- def
OAI.RegularPointCoordinates.cutoffHeatWeightline 27Source documentation
The actual cutoff heat weight, as a bounded continuous function.
def cutoffHeatWeight {t : ℝ} (ht : 0 < t) (x : X) : X →ᵇ ℝ := … - theorem
OAI.RegularPointCoordinates.cutoffHeatWeight_applyline 33 - def
OAI.RegularPointCoordinates.cutoffHeatMassline 40Source documentation
Heat integration of the full mass measure on a finite coordinate span.
def cutoffHeatMass {t : ℝ} (ht : 0 < t) (x : X) : E →L[ℝ] E := … - theorem
OAI.RegularPointCoordinates.cutoffHeatMass_energyline 43 - theorem
OAI.RegularPointCoordinates.cutoffHeatMass_isPositiveline 48 - theorem
OAI.RegularPointCoordinates.cutoffHeatMass_comapline 54 - theorem
OAI.RegularPointCoordinates.cutoffHeatMass_lower_massline 61Source documentation
Kernel lower estimates turn directly into estimates for singular or absolutely continuous mass on the testing ball.
theorem cutoffHeatMass_lower_mass (hχpos : ∀ y, 0 ≤ χ y) {t : ℝ} (ht : 0 < t) (x : X) (s : Set X) (hs : MeasurableSet s) (hχone : ∀ y ∈ s, χ y = 1) (c : ℝ) (hc : ∀ y ∈ s, c ≤ p t x y) (v : E) : c * ⟪v, M.massOperator s v⟫_ℝ ≤ ⟪v, cutoffHeatMass μ hQ hp hχ hsχ M ht x v⟫_ℝ := by … - theorem
OAI.RegularPointCoordinates.cutoffHeatMass_energy_monoline 74Source documentation
Spatial comparisons of the kernel also compare heat mass matrices, without needing pointwise representatives of a mass density.
theorem cutoffHeatMass_energy_mono (hχpos : ∀ y, 0 ≤ χ y) {t s : ℝ} (ht : 0 < t) (hs : 0 < s) (x z : X) (hkernel : ∀ y, p t x y ≤ p s z y) (v : E) : ⟪v, cutoffHeatMass μ hQ hp hχ hsχ M ht x v⟫_ℝ ≤ ⟪v, cutoffHeatMass μ hQ hp hχ hsχ M hs z v⟫_ℝ := by …