Documentation

LeanPool.CaffarelliKohnNirenberg.Foundation.Euclidean.RieszSecond

Riesz Second #

Part of the Caffarelli–Kohn–Nirenberg partial regularity proof.

The Euclidean 2√3 enlargement of a dyadic cube, with the cube's sup-radius dyadicScale Q.scale / 2.

Equations
  • One or more equations did not get rendered due to their size.
Instances For

    The enlarged cube has the explicit volume comparison needed in the bad region estimate.

    theorem CKN.Foundation.Euclidean.rieszSecond_good_part_chebyshev {F : Parabolic.Vec3 → ℝ} {height level C A : ℝ} (D : CZDecomposition F height) (hheight : 0 < height) (hlevel : 0 < level) (hA : 0 ≤ A) (henergy : ∫ (x : Parabolic.Vec3), dyadicGoodPart F D.cubes x ^ 2 ≤ 8 * height * A) {T : Parabolic.Vec3 → ℝ → ℝ} (hT : MeasureTheory.Integrable (fun (x : Parabolic.Vec3) => T x (dyadicGoodPart F D.cubes x) ^ 2) MeasureTheory.volume) (hL2 : ∫ (x : Parabolic.Vec3), T x (dyadicGoodPart F D.cubes x) ^ 2 ≤ C ^ 2 * ∫ (x : Parabolic.Vec3), dyadicGoodPart F D.cubes x ^ 2) :

    The good part estimate after the (L^2) operator bound and Chebyshev.

    The summed bad-part estimate supplied by the Hörmander integral bound.

    theorem CKN.Foundation.Euclidean.rieszSecond_weak_type_unconditional {F : Parabolic.Vec3 → ℝ} {level C₂ A : ℝ} {C_H : ENNReal} (hF : MeasureTheory.Integrable F MeasureTheory.volume) (hlevel : 0 < level) (hA : 0 ≤ A) (hAeq : dyadicL1Norm F = ENNReal.ofReal A) {T : Parabolic.Vec3 → ℝ} {G B : CZDecomposition F level → Parabolic.Vec3 → ℝ} (hdecomp : ∀ (D : CZDecomposition F level) (x : Parabolic.Vec3), T x = G D x + B D x) (henergy : ∀ (D : CZDecomposition F level), ∫ (x : Parabolic.Vec3), dyadicGoodPart F D.cubes x ^ 2 ≤ 8 * level * A) (hL2 : ∀ (D : CZDecomposition F level), MeasureTheory.Integrable (fun (x : Parabolic.Vec3) => G D x ^ 2) MeasureTheory.volume ∧ ∫ (x : Parabolic.Vec3), G D x ^ 2 ≤ C₂ ^ 2 * ∫ (x : Parabolic.Vec3), dyadicGoodPart F D.cubes x ^ 2) (hbad : ∀ (D : CZDecomposition F level), ∃ (Tbad : { Q : DyadicIndex // Q ∈ D.cubes } → Parabolic.Vec3 → ℝ), MeasureTheory.Integrable (B D) MeasureTheory.volume ∧ (∀ᵐ (x : Parabolic.Vec3) ∂MeasureTheory.volume.restrict (⋃ (Q : { Q : DyadicIndex // Q ∈ D.cubes }), rieszSecondCubeStar ↑Q)ᶜ, ENNReal.ofReal |B D x| ≤ ∑' (Q : { Q : DyadicIndex // Q ∈ D.cubes }), ENNReal.ofReal |Tbad Q x|) ∧ (∀ (Q : { Q : DyadicIndex // Q ∈ D.cubes }), AEMeasurable (fun (x : Parabolic.Vec3) => ENNReal.ofReal |Tbad Q x|) (MeasureTheory.volume.restrict (⋃ (Q : { Q : DyadicIndex // Q ∈ D.cubes }), rieszSecondCubeStar ↑Q)ᶜ)) ∧ ∀ (Q : { Q : DyadicIndex // Q ∈ D.cubes }), ∫⁻ (x : Parabolic.Vec3) in (rieszSecondCubeStar ↑Q)ᶜ, ENNReal.ofReal |Tbad Q x| ≤ C_H * ∫⁻ (x : Parabolic.Vec3) in dyadicCubeSet ↑Q, ENNReal.ofReal |dyadicBadPart F (↑Q) x|) :