Quadratic energy on the normalized cylinder

Finite weak derivative data give an integrable quadratic energy for the Gaussian unique continuation argument.

theorem ESS.uc_normalized_energy_integrable {ρ : ℝ} {v : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3} {Dv : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3} {D2v : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3} {Dtv : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3} (hweak : CKN.HasSpaceTimeWeakDerivs (CKN.Foundation.Parabolic.vec3Ball 0 ρ) (Set.Ioo 0 2) v Dv D2v Dtv) (hL2 : ∫⁻ (z : CKN.Foundation.Parabolic.ParabolicPoint) in ucCylinder ρ, ‖v z‖ₑ ^ 2 + ‖Dv z‖ₑ ^ 2 + ‖D2v z‖ₑ ^ 2 + ‖Dtv z‖ₑ ^ 2 < ⊤) : MeasureTheory.IntegrableOn (fun (z : CKN.Foundation.Parabolic.ParabolicPoint) => CKN.Foundation.Parabolic.vec3EuclideanNorm (v z) ^ 2) (ucCylinder ρ) MeasureTheory.volume ∧ MeasureTheory.IntegrableOn (fun (z : CKN.Foundation.Parabolic.ParabolicPoint) => CKN.spatialGradientSq v Dv z) (ucCylinder ρ) MeasureTheory.volume

Finite quadratic weak derivative data give an integrable normalized field and spatial gradient energy.