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LeanPool.CaffarelliKohnNirenberg.Pressure.PkBoundsP56

Pk Bounds P56 #

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

Fixed-time annular estimates for the pressure and cutoff terms.

theorem CKN.pressureP56_pointwise_annular_bound {η : Foundation.Parabolic.Vec3 → ℝ} {p : Foundation.Parabolic.ParabolicPoint → ℝ} {x₀ : Foundation.Parabolic.Vec3} {ρ r s C₁ C₂ : ℝ} (hρ : 0 < ρ) :
0 ≤ C₁ → ∀ (hC₂ : 0 ≤ C₂) (hp : MeasureTheory.Integrable (fun (y : Foundation.Parabolic.Vec3) => |p (y, s)|) (MeasureTheory.volume.restrict (Foundation.Parabolic.vec3Ball x₀ ρ))) (hLap : ∀ (y : Foundation.Parabolic.Vec3), |spatialLaplacian η y| ≤ C₂ / ρ ^ 2) (hD₁ : ∀ (j : Fin 3) (y : Foundation.Parabolic.Vec3), |spatialDeriv η j y| ≤ C₁ / ρ) (hI₅ : MeasureTheory.Integrable (fun (y : Foundation.Parabolic.Vec3) => p (y, s) * spatialLaplacian η y) MeasureTheory.volume) (hP₅ : ∀ {x : Foundation.Parabolic.Vec3}, x ∈ Foundation.Parabolic.vec3Ball x₀ r → MeasureTheory.Integrable (fun (y : Foundation.Parabolic.Vec3) => -Foundation.Heat.newtonianKernel (x - y) * (p (y, s) * spatialLaplacian η y)) MeasureTheory.volume) (hA₅ : ∀ (y : Foundation.Parabolic.Vec3), p (y, s) * spatialLaplacian η y ≠ 0 → y ∈ pressureAnnulus x₀ ρ) (hI₆ : ∀ (j : Fin 3), MeasureTheory.Integrable (fun (y : Foundation.Parabolic.Vec3) => spatialDeriv η j y * p (y, s)) MeasureTheory.volume) (hP₆ : ∀ (j : Fin 3) {x : Foundation.Parabolic.Vec3}, x ∈ Foundation.Parabolic.vec3Ball x₀ r → MeasureTheory.Integrable (fun (y : Foundation.Parabolic.Vec3) => spatialDeriv Foundation.Heat.newtonianKernel j (x - y) * (spatialDeriv η j y * p (y, s))) MeasureTheory.volume) (hA₆ : ∀ (j : Fin 3) (y : Foundation.Parabolic.Vec3), spatialDeriv η j y * p (y, s) ≠ 0 → y ∈ pressureAnnulus x₀ ρ) (hr : 0 < r) (hhalf : r ≤ ρ / 2) {x : Foundation.Parabolic.Vec3} (hx : x ∈ Foundation.Parabolic.vec3Ball x₀ r), |pressureP5 η p s x| + |pressureP6 η p s x| ≤ (6 * C₂ + 240 * C₁) / ρ ^ 3 * ∫ (y : Foundation.Parabolic.Vec3) in Foundation.Parabolic.vec3Ball x₀ ρ, |p (y, s)|