Harmonic Part Bounds AE #
Part of the Caffarelli–Kohn–Nirenberg partial regularity proof.
theorem
CKN.exists_harmonicPressurePart_Ck_ae_of_sws
(k : ℕ)
:
∃ (C₁₆ : ℝ),
0 ≤ C₁₆ ∧ ∀ {Ω : Set Foundation.Parabolic.Vec3} {I : Set ℝ} {q : ℝ}
{u : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3}
{Du : Foundation.Parabolic.ParabolicPoint → Fin 3 → Foundation.Parabolic.Vec3}
{p : Foundation.Parabolic.ParabolicPoint → ℝ}
{f : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3},
IsSuitableWeakSolutionIntegrable Ω I q u Du p f →
∀ {z : Foundation.Parabolic.ParabolicPoint} {ρ : ℝ} (hρ : 0 < ρ),
closure (Foundation.Parabolic.parabolicCylinder z.1 z.2 ρ) ⊆ spaceTimeSet Ω I →
∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioc (z.2 - ρ ^ 2) z.2), ∀ x ∈ Foundation.Parabolic.vec3Ball z.1 (ρ / 2),
‖iteratedFDeriv ℝ k
(harmonicPressurePart (mollifiedBallCutoff z.1 hρ) u
(fun (t : ℝ) (j : Fin 3) =>
⨍ (y : Foundation.Parabolic.Vec3) in Foundation.Parabolic.vec3Ball z.1 ρ, u (y, t) j)
p s)
x‖ ≤ C₁₆ * ρ ^ (-(2 + ↑k)) * (alpha u z ρ ^ 2 + MeasureTheory.lpNorm (fun (y : Foundation.Parabolic.Vec3) => p (y, s)) (ENNReal.ofReal (3 / 2))
(MeasureTheory.volume.restrict (Foundation.Parabolic.vec3Ball z.1 ρ)))