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LeanPool.CaffarelliKohnNirenberg.Core.Step4.SliceSelectedGradientSWSUnconditional

Display (3.5) on a slice, with no condition on the divergence of the force #

Display (3.5) of the pressure-gradient section selects, for almost every time of the one-sided interval J_ρ, a weak spatial gradient of the pressure slice on the half ball B_{ρ/2}(x₀) together with its L^{6/5} bound. The general form of that selection carries three analytic hypotheses: the interior regularity of the harmonic part of the local pressure decomposition, the first-order identification of the first pressure potential, and the weak gradient of the two force potentials.

The class def:sws imposes no condition on the spatial divergence of the force, so the two force potentials of eq:pk do not cancel and the display must carry them. This file discharges the first hypothesis outright, reduces the second to the divergence-form characterization of the slice source V, and discharges the third from the force data of the solution alone: the bound gains the ρ^{-1/2}-weighted force term sliceForceGradientBound.

theorem CKN.Core.Step4.slice_selected_gradient_ae_of_sws_of_source_data_unconditional_with_hP1 (C_CZ C₁₇ C₁₁ C₈ : ℝ) (hC_CZ : 0 ≤ C_CZ) (hC₁₇ : 1000 * Foundation.Heat.harmonicInteriorDisplayConstant ≤ C₁₇) (hC₈ : sliceForceGradientConstant ≤ C₈) {E F : ℝ → ℝ} {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 V : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3} (hsol : IsSuitableWeakSolutionIntegrable Ω I q u Du p f) {z : Foundation.Parabolic.ParabolicPoint} {ρ : ℝ} (hρ : 0 < ρ) (hsub : closure (Foundation.Parabolic.parabolicCylinder z.1 z.2 ρ) ⊆ spaceTimeSet Ω I) (hC₁₁ : 0 ≤ C₁₁) (hE : ∀ (s : ℝ), 0 ≤ E s) (hF : ∀ (s : ℝ), 0 ≤ F s) (hP1 : ∀ (i : Fin 3) (G : Foundation.Parabolic.Vec3 → ℝ), MeasureTheory.MemLp G (ENNReal.ofReal (6 / 5)) MeasureTheory.volume → HasCompactSupport G → ∃ (D : Foundation.Parabolic.Vec3 → Foundation.Parabolic.Vec3), MeasureTheory.MemLp D (ENNReal.ofReal (6 / 5)) MeasureTheory.volume ∧ (∀ (j : Fin 3) (ψ : Foundation.Parabolic.Vec3 → ℝ), ContDiff ℝ (↑⊤) ψ → HasCompactSupport ψ → ∫ (x : Foundation.Parabolic.Vec3), pressureNewtonianDerivativePotential i G x * spatialDeriv ψ j x = -∫ (x : Foundation.Parabolic.Vec3), D x j * ψ x) ∧ MeasureTheory.eLpNorm D (ENNReal.ofReal (6 / 5)) MeasureTheory.volume ≤ ENNReal.ofReal C_CZ * MeasureTheory.eLpNorm G (ENNReal.ofReal (6 / 5)) MeasureTheory.volume) (hCZ_p1 : ∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioc (z.2 - ρ ^ 2) z.2), MeasureTheory.MemLp (pressureP1 (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 f s) (ENNReal.ofReal (3 / 2)) MeasureTheory.volume ∧ MeasureTheory.lpNorm (pressureP1 (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 f s) (ENNReal.ofReal (3 / 2)) MeasureTheory.volume ≤ C₁₁ * E s ^ (2 / 3)) (hP78 : ∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioc (z.2 - ρ ^ 2) z.2), MeasureTheory.MemLp (pressureP7 (mollifiedBallCutoff z.1 hρ) f s + pressureP8 (mollifiedBallCutoff z.1 hρ) f s) (ENNReal.ofReal (3 / 2)) (MeasureTheory.volume.restrict (euclideanBall z.1 (13 * ρ / 20))) ∧ MeasureTheory.lpNorm (pressureP7 (mollifiedBallCutoff z.1 hρ) f s + pressureP8 (mollifiedBallCutoff z.1 hρ) f s) (ENNReal.ofReal (3 / 2)) (MeasureTheory.volume.restrict (euclideanBall z.1 (13 * ρ / 20))) ≤ F s) (hV : ∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioc (z.2 - ρ ^ 2) z.2), (∀ (i : Fin 3), MeasureTheory.MemLp (fun (x : Foundation.Parabolic.Vec3) => V (x, s) i) (ENNReal.ofReal (6 / 5)) MeasureTheory.volume) ∧ ∀ (i : Fin 3), HasCompactSupport fun (x : Foundation.Parabolic.Vec3) => V (x, s) i) (hVpair : ∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioc (z.2 - ρ ^ 2) z.2), ∀ (ψ : Foundation.Parabolic.Vec3 → ℝ), ContDiff ℝ (↑⊤) ψ → HasCompactSupport ψ → ∑ i : Fin 3, ∫ (x : Foundation.Parabolic.Vec3), V (x, s) i * spatialDeriv ψ i x = pressureSecondPairing (fun (i j : Fin 3) (x : Foundation.Parabolic.Vec3) => mollifiedBallCutoff z.1 hρ x * pressureUTensor u (fun (t : ℝ) (j : Fin 3) => ⨍ (y : Foundation.Parabolic.Vec3) in Foundation.Parabolic.vec3Ball z.1 ρ, u (y, t) j) (x, s) i j) ψ) :
∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioc (z.2 - ρ ^ 2) z.2), ∃ (D : Foundation.Parabolic.Vec3 → Foundation.Parabolic.Vec3), (∀ (k : Fin 3), MeasureTheory.LocallyIntegrableOn (fun (x : Foundation.Parabolic.Vec3) => D x k) (euclideanBall z.1 (ρ / 2)) MeasureTheory.volume) ∧ MeasureTheory.MemLp D (ENNReal.ofReal (6 / 5)) (MeasureTheory.volume.restrict (euclideanBall z.1 (ρ / 2))) ∧ (∀ (k : Fin 3), HasWeakPartialDerivOn (euclideanBall z.1 (ρ / 2)) k (fun (x : Vec 3) => p (x, s)) fun (x : Vec 3) => D x k) ∧ ∀ (k : Fin 3), MeasureTheory.eLpNorm (fun (x : Foundation.Parabolic.Vec3) => D x k) (ENNReal.ofReal (6 / 5)) (MeasureTheory.volume.restrict (euclideanBall z.1 (ρ / 2))) ≤ ENNReal.ofReal C_CZ * ∑ i : Fin 3, MeasureTheory.eLpNorm (fun (x : Foundation.Parabolic.Vec3) => V (x, s) i) (ENNReal.ofReal (6 / 5)) MeasureTheory.volume + ENNReal.ofReal (C₁₇ * (MeasureTheory.lpNorm (fun (x : Foundation.Parabolic.Vec3) => p (x, s)) (ENNReal.ofReal (3 / 2)) (MeasureTheory.volume.restrict (euclideanBall z.1 ρ)) + C₁₁ * E s ^ (2 / 3) + F s) * ρ ^ (-1 / 2)) + ENNReal.ofReal (sliceForceGradientBound C_CZ C₈ z.1 hρ f s)

Conditional display (3.5) on a slice of a suitable weak solution. The weak-gradient construction hP1 remains an explicit input; the interior regularity of the harmonic part, first-order identification, and force slot are discharged from the solution data, with no condition on the divergence of the force.

Almost every slice of the pressure has a Vec3-valued weak spatial gradient on B_{ρ/2}(x₀), in L^{6/5} there, bounded by the Calderón–Zygmund norm of the divergence-form source, the ρ^{-1/2}-weighted L^{3/2} norm of the pressure, and the force term of the display.