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LeanPool.CaffarelliKohnNirenberg.Core.Step4.PressureGradientOriginClauseDerivativeLocal

Fixed derivative decomposition on backward local cylinders #

The fixed-source construction is applied on an arbitrary backward cylinder, including cylinders ending at the final carrier time. The source argument specializes the same-repository fixed-source Morrey estimates to this geometry. The selected derivative is retained in the signed Riesz and remainder identity.

theorem CKN.Core.Step4.originClause_local_derivative_morrey_of_remainder {τ q : ℝ} (hq : 5 / 2 < q) (hτ : 25 / 3 ≤ τ) (hτhi : τ ≤ 25) {Ω : Set Foundation.Parabolic.Vec3} {I : Set 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} {z : Foundation.Parabolic.ParabolicPoint} {ρ : ℝ} (hρ : 0 < ρ) (hrem : ∃ (M : ℝ → ENNReal), AEMeasurable M MeasureTheory.volume ∧ ∫⁻ (s : ℝ), M s ^ (3 / 2) < ⊤ ∧ ∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioc (z.2 - ρ ^ 2) z.2), ∀ (i : Fin 3), ∀ x ∈ Foundation.Parabolic.vec3Ball z.1 (ρ / 2), ‖classicalGradient (harmonicPressurePart (mollifiedBallCutoff z.1 hρ) u (sourceSliceCentredMean z.1 ρ u) p s + pressureP8 (mollifiedBallCutoff z.1 hρ) f s) x i‖ₑ ≤ M s) (hsol : IsSuitableWeakSolutionIntegrable Ω I q u Du p f) (hsub : closure (Foundation.Parabolic.parabolicCylinder z.1 z.2 ρ) ⊆ spaceTimeSet Ω I) (hbox : localBox Ω I (Foundation.Parabolic.vec3Ball z.1 ρ) (Set.Ioc (z.2 - ρ ^ 2) z.2)) (hU : ∀ (j : Fin 3), Foundation.Parabolic.Morrey.morreyNorm 3 τ ((Foundation.Parabolic.parabolicCylinder z.1 z.2 ρ).indicator fun (w : Foundation.Parabolic.ParabolicPoint) => u w j) < ⊤) (hD : ∀ (j k : Fin 3), Foundation.Parabolic.Morrey.morreyNorm 2 (25 / 8) ((Foundation.Parabolic.parabolicCylinder z.1 z.2 ρ).indicator fun (w : Foundation.Parabolic.ParabolicPoint) => Du w j k) < ⊤) {Dp : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3} (hDp : Measurable Dp) (hweak : ∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioc (z.2 - ρ ^ 2) z.2), ∀ (i : Fin 3), MeasureTheory.LocallyIntegrableOn (fun (y : Foundation.Parabolic.Vec3) => Dp (y, s) i) (Foundation.Parabolic.vec3Ball z.1 (ρ / 2)) MeasureTheory.volume ∧ HasWeakPartialDerivOn (Foundation.Parabolic.vec3Ball z.1 (ρ / 2)) i (fun (y : Vec 3) => p (y, s)) fun (y : Vec 3) => Dp (y, s) i) (i : Fin 3) :
Foundation.Parabolic.Morrey.morreyNorm (6 / 5) (min (1 / τ + 8 / 25)⁻¹ q) ((Foundation.Parabolic.vec3Ball z.1 (ρ / 2) ×ˢ Set.Ioc (z.2 - ρ ^ 2) z.2).indicator fun (w : Foundation.Parabolic.Vec3 × ℝ) => Dp w i) < ⊤

On one backward cylinder, the fixed harmonic/far temporal envelope gives Morrey control of the same selected weak derivative on its spatial half-ball. The source and force classes are derived from suitability and the stated velocity and gradient Morrey data on the localization cylinder.