OAI/Geometry/RCD/Sobolev/PositiveSourceTail.lean
2 declarations, 0 contain sorry, 0 declared as axioms
Power tails from the actual Dirichlet truncation test
This is the Sobolev step in the positive-source estimate. The measure bound is derived from clipped moments and then applied to genuine Dirichlet functions with a bounded positive source functional.
- theorem
OAI.RegularPointCoordinates.power_tail_of_clip_momentline 22Source documentation
The clipped Sobolev moment inequality implies the weak power tail.
theorem power_tail_of_clip_moment {X : Type*} [MeasurableSpace X] (ν : Measure X) [IsFiniteMeasure ν] {H : X → ℝ} (hH : Measurable H) {d C : ℝ} (hd : 0 < d) (hC : 0 ≤ C) (hclip : ∀ t : ℝ, 0 < t → (∫ x, (positiveClip t (H x)) ^ (2 * d) ∂ν) ^ (1 / d) ≤ C * t) {t : ℝ} (ht : 0 < t) : ν {x | t ≤ H x} ≤ ENNReal.ofReal (C ^ d * t ^ (-d)) := by …Mentions: OAI.RegularPointCoordinates.positiveClip
- theorem
OAI.RegularPointCoordinates.dirichlet_positive_source_tailline 72Source documentation
The weak power tail for a positive-source Dirichlet solution. The Sobolev inequality and source bound are stated separately, on the actual Dirichlet space. The desired tail is derived rather than postulated.
theorem dirichlet_positive_source_tail (Ω : Set X) (hΩfin : μ Ω ≠ ∞) (H : SobolevSpace.dirichlet μ hQ Ω) (hH : ∀ᵐ x ∂μ, 0 ≤ SobolevSpace.toLp μ hQ H.val x) {d C P : ℝ} (hd : 0 < d) (hC : 0 ≤ C) (hP : 0 ≤ P) (hsob : ∀ φ : SobolevSpace.dirichlet μ hQ Ω, (∫ x in Ω, |SobolevSpace.toLp μ hQ φ.val x| ^ (2 * d) ∂μ) ^ (1 / d) ≤ C * energyForm μ hQ φ.val φ.val) (hsource : ∀ φ : SobolevSpace.dirichlet μ hQ Ω, ∀ s : ℝ, 0 ≤ s → (∀ᵐ x ∂μ, 0 ≤ SobolevSpace.toLp μ hQ φ.val x ∧ SobolevSpace.toLp μ hQ φ.val x ≤ s) → energyForm μ hQ H.val φ.val ≤ P * s) {t : ℝ} (ht : 0 < t) : (μ.restrict Ω) {x | t ≤ SobolevSpace.toLp μ hQ H.val x} ≤ …Mentions: OAI.RegularPointCoordinates.SobolevSpace.dirichlet, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.energyForm