OAI/Geometry/RCD/Heat/FiniteHeatMassShells.lean
3 declarations, 0 contain sorry, 0 declared as axioms
Finite shell bounds for the full Bochner heat mass
- theorem
OAI.RegularPointCoordinates.finite_dyadicShell_unionline 19Source documentation
The first N+1 shells partition exactly the corresponding outer ball.
theorem finite_dyadicShell_union (p : X) {r : ℝ} (hr : 0 ≤ r) (N : ℕ) : (⋃ j ∈ Finset.range (N + 1), dyadicShell p r j) = ball p (2 ^ N * r) := by …Mentions: OAI.RegularPointCoordinates.dyadicShell
- theorem
OAI.RegularPointCoordinates.integral_le_finite_shell_massline 30Source documentation
Integrate finitely many controlled shells and use a single bound on the exterior. This applies directly to singular finite mass measures.
theorem integral_le_finite_shell_mass (ν : Measure X) [IsFiniteMeasure ν] (p : X) {r : ℝ} (hr : 0 ≤ r) (N : ℕ) {f : X → ℝ} (hf : Integrable f ν) (W : ℕ → ℝ) (hW : ∀ j, 0 ≤ W j) (hlocal : ∀ j ≤ N, ∀ᵐ z ∂ν.restrict (dyadicShell p r j), f z ≤ W j) {T : ℝ} (hT : 0 ≤ T) (htail : ∀ᵐ z ∂ν.restrict (ball p (2 ^ N * r))ᶜ, f z ≤ T) : (∫ z, f z ∂ν) ≤ (∑ j ∈ Finset.range (N + 1), W j * ν.real (ball p (2 ^ j * r))) + T * ν.real univ := by …Mentions: OAI.RegularPointCoordinates.dyadicShell
- theorem
OAI.RegularPointCoordinates.cutoffHeatMass_le_finite_shellsline 63Source documentation
The shell bound controls the actual heat mass of the full positive Bochner measure, not just an assumed density.
theorem cutoffHeatMass_le_finite_shells (M : PositiveBilinearMeasure X E) (p : X) {r t : ℝ} (hr : 0 ≤ r) (ht : 0 < t) (N : ℕ) (W : ℕ → ℝ) (hW : ∀ j, 0 ≤ W j) (hlocal : ∀ j ≤ N, ∀ z ∈ dyadicShell p r j, χ z * ker t p z ≤ W j) {T : ℝ} (hT : 0 ≤ T) (htail : ∀ z ∉ ball p (2 ^ N * r), χ z * ker t p z ≤ T) (v : E) : ⟪v, cutoffHeatMass μ hQ hk hχ hsχ M ht p v⟫_ℝ ≤ (∑ j ∈ Finset.range (N + 1), W j * (M.measure v).real (ball p (2 ^ j * r))) + T * (M.measure v).real univ := by …Mentions: OAI.RegularPointCoordinates.PositiveBilinearMeasure, OAI.RegularPointCoordinates.dyadicShell, OAI.RegularPointCoordinates.cutoffHeatMass