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LeanPool.CaffarelliKohnNirenberg.Core.Step4.SliceSelectedGradientAssembly

The selected weak pressure gradient on one slice #

Display (3.5) of the pressure-gradient section estimates the weak spatial gradient of a pressure slice after the local decomposition p = p₁ + p_har + (p₇ + p₈). The first summand is a coordinate sum of Newtonian derivative potentials of a divergence-form source V and is differentiated by the Calderón–Zygmund selection; the second is smooth on the inner ball and is differentiated classically; the third is differentiated by its own potential identities.

This file performs the assembly: it produces one Vec3-valued slice field whose coordinates are locally integrable, which lies in L^{6/5} on the inner set, which is the coordinate weak gradient of the pressure slice there, and whose coordinate norms obey the three-term bound of display (3.5).

Each coordinate of a globally L^{6/5} vector field is locally integrable on every set. This is the local integrability that display (3.5) requires of the Calderón–Zygmund part of the selected gradient.

theorem CKN.Core.Step4.slice_selected_gradient_of_potential_representation (C_CZ : ℝ) {Sh Sw : ENNReal} (hSh : Sh ≠ ⊤) (hSw : Sw ≠ ⊤) {B B' : Set Foundation.Parabolic.Vec3} (hB : IsOpen B) {p h w : Foundation.Parabolic.Vec3 → ℝ} {V : Foundation.Parabolic.Vec3 → Foundation.Parabolic.Vec3} {gw : Fin 3 → Foundation.Parabolic.Vec3 → ℝ} (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) (hV : ∀ (i : Fin 3), MeasureTheory.MemLp (fun (x : Foundation.Parabolic.Vec3) => V x i) (ENNReal.ofReal (6 / 5)) MeasureTheory.volume) (hVc : ∀ (i : Fin 3), HasCompactSupport fun (x : Foundation.Parabolic.Vec3) => V x i) (hrep : p =ᵐ[MeasureTheory.volume.restrict B] fun (x : Foundation.Parabolic.Vec3) => ∑ i : Fin 3, pressureNewtonianDerivativePotential i (fun (y : Foundation.Parabolic.Vec3) => V y i) x + (h x + w x)) (hh : ContDiffOn ℝ (↑1) h B) (hhbound : ∀ (k : Fin 3), MeasureTheory.eLpNorm (fun (x : Vec 3) => classicalGradient h x k) (ENNReal.ofReal (6 / 5)) (MeasureTheory.volume.restrict B') ≤ Sh) (hwloc : MeasureTheory.LocallyIntegrableOn w B MeasureTheory.volume) (hw : ∀ (k : Fin 3), HasWeakPartialDerivOn B k w (gw k)) (hgwloc : ∀ (k : Fin 3), MeasureTheory.LocallyIntegrableOn (gw k) B MeasureTheory.volume) (hgwbound : ∀ (k : Fin 3), MeasureTheory.eLpNorm (gw k) (ENNReal.ofReal (6 / 5)) (MeasureTheory.volume.restrict B') ≤ Sw) :

The one-slice assembly behind display (3.5) of the pressure-gradient section.

On an open set B the pressure slice p agrees almost everywhere with the sum of the coordinate Newtonian derivative potentials of a compactly supported L^{6/5} source V, of a function h which is C¹ on B, and of a function w carrying its own coordinate weak derivatives gw. The Calderón–Zygmund selection hP1 supplies the weak gradient of the potential part together with its L^{6/5} bound. The conclusion is a single field D whose coordinates are locally integrable on B, which lies in L^{6/5} on B', which is the coordinate weak gradient of p on B, and which obeys the three-term bound of display (3.5).

The coordinate sum of source norms appearing in the assembled bound is controlled by the norm of the source on the ball carrying its support, which is the form of the first term of display (3.5). The factor three is the number of spatial coordinates.

The assembled bound rewritten with the source norm taken on the ball carrying the support of the source, which is the first term of display (3.5). The three spatial coordinates are absorbed into the constant.