Numerical bounds for the first Morrey improvement #
The constants in Adams' estimate and in lowering the integrability exponent are retained. This gives a bound determined by the source bounds, not by a new existential constant chosen after the solution.
The order-two Adams coefficient after lowering integrability to three.
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The order-one Adams coefficient after lowering integrability to three.
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The numerical velocity bound determined by the two source bounds.
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theorem
CKN.Core.Endgame.potential_majorant_morrey_le
(KF KG : ENNReal)
{g : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3}
{h : Fin 3 → Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3}
(hg : ∀ (i : Fin 3), AEMeasurable (fun (z : Foundation.Parabolic.ParabolicPoint) => g z i) MeasureTheory.volume)
(hh : ∀ (j i : Fin 3), AEMeasurable (fun (z : Foundation.Parabolic.ParabolicPoint) => h j z i) MeasureTheory.volume)
(hNF :
(Foundation.Parabolic.Morrey.morreyNorm (6 / 5) (25 / 11) fun (z : Foundation.Parabolic.ParabolicPoint) =>
Foundation.Parabolic.vec3EuclideanNorm (g z)) ≤ KF)
(hNG :
∀ (j : Fin 3),
(Foundation.Parabolic.Morrey.morreyNorm 3 (25 / 6) fun (z : Foundation.Parabolic.ParabolicPoint) =>
Foundation.Parabolic.vec3EuclideanNorm (h j z)) ≤ KG)
:
The potential majorant retains an explicit bound from the source bounds.
theorem
CKN.Core.Endgame.bootstrap_morrey_le_of_sources
(KF KG : ENNReal)
(hKF : KF < ⊤)
(hKG : KG < ⊤)
{v g : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3}
{h : Fin 3 → Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3}
{z₀ : Foundation.Parabolic.ParabolicPoint}
{R : ℝ}
(hR : 0 < R)
(hg : ∀ (i : Fin 3), AEMeasurable (fun (z : Foundation.Parabolic.ParabolicPoint) => g z i) MeasureTheory.volume)
(hh : ∀ (j i : Fin 3), AEMeasurable (fun (z : Foundation.Parabolic.ParabolicPoint) => h j z i) MeasureTheory.volume)
(hNF :
(Foundation.Parabolic.Morrey.morreyNorm (6 / 5) (25 / 11) fun (z : Foundation.Parabolic.ParabolicPoint) =>
Foundation.Parabolic.vec3EuclideanNorm (g z)) ≤ KF)
(hNG :
∀ (j : Fin 3),
(Foundation.Parabolic.Morrey.morreyNorm 3 (25 / 6) fun (z : Foundation.Parabolic.ParabolicPoint) =>
Foundation.Parabolic.vec3EuclideanNorm (h j z)) ≤ KG)
(hgsupp : ∀ z ∉ Foundation.Parabolic.parabolicCylinder z₀.1 z₀.2 R, g z = 0)
(hhsupp : ∀ (j : Fin 3), ∀ z ∉ Foundation.Parabolic.parabolicCylinder z₀.1 z₀.2 R, h j z = 0)
(hrep : v =ᵐ[MeasureTheory.volume] Step3.duhamelPotential g h)
:
(Foundation.Parabolic.Morrey.morreyNorm 3 25 fun (z : Foundation.Parabolic.ParabolicPoint) =>
Foundation.Parabolic.vec3EuclideanNorm (v z)) ≤ bootstrapSourceMorreyBound KF KG
The first Morrey improvement has a source-uniform numerical bound. Actual kernel finiteness is derived before applying the real majorant.
theorem
CKN.Core.Endgame.bootstrap_morrey_le_of_component_sources
(KF KG : ENNReal)
(hKF : KF < ⊤)
(hKG : KG < ⊤)
{v g : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3}
{h : Fin 3 → Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3}
{z₀ : Foundation.Parabolic.ParabolicPoint}
{R : ℝ}
(hR : 0 < R)
(hg : ∀ (i : Fin 3), AEMeasurable (fun (z : Foundation.Parabolic.ParabolicPoint) => g z i) MeasureTheory.volume)
(hh : ∀ (j i : Fin 3), AEMeasurable (fun (z : Foundation.Parabolic.ParabolicPoint) => h j z i) MeasureTheory.volume)
(hNF :
∀ (i : Fin 3),
(Foundation.Parabolic.Morrey.morreyNorm (6 / 5) (25 / 11) fun (z : Foundation.Parabolic.ParabolicPoint) => g z i) ≤ KF)
(hNG :
∀ (j i : Fin 3),
(Foundation.Parabolic.Morrey.morreyNorm 3 (25 / 6) fun (z : Foundation.Parabolic.ParabolicPoint) => h j z i) ≤ KG)
(hgsupp : ∀ z ∉ Foundation.Parabolic.parabolicCylinder z₀.1 z₀.2 R, g z = 0)
(hhsupp : ∀ (j : Fin 3), ∀ z ∉ Foundation.Parabolic.parabolicCylinder z₀.1 z₀.2 R, h j z = 0)
(hrep : v =ᵐ[MeasureTheory.volume] Step3.duhamelPotential g h)
:
(Foundation.Parabolic.Morrey.morreyNorm 3 25 fun (z : Foundation.Parabolic.ParabolicPoint) =>
Foundation.Parabolic.vec3EuclideanNorm (v z)) ≤ bootstrapSourceMorreyBound (3 * KF) (3 * KG)
Componentwise source bounds supply the numerical bootstrap bound with the explicit three-coordinate aggregation factor.