Quadratic weak-derivative data under scaling #
The parabolic dilation used in lem:uc-gaussian preserves finite quadratic
energy on the normalized cylinder.
theorem
ESS.uc_scaled_l2_data
(x₀ : CKN.Foundation.Parabolic.Vec3)
(R T scale ρ : ℝ)
(hscale : 0 < scale)
(hscale1 : scale ≤ 1)
(hball : scale * ρ ≤ R)
(htime : 2 * scale ^ 2 ≤ T)
(w : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Dw : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(D2w : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(Dtw : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(hweak : CKN.HasSpaceTimeWeakDerivs (CKN.Foundation.Parabolic.vec3Ball x₀ R) (Set.Ioo 0 T) w Dw D2w Dtw)
(hL2 :
∫⁻ (z : CKN.Foundation.Parabolic.ParabolicPoint) in CKN.spaceTimeSet (CKN.Foundation.Parabolic.vec3Ball x₀ R) (Set.Ioo 0 T), ‖w z‖ₑ ^ 2 + ‖Dw z‖ₑ ^ 2 + ‖D2w z‖ₑ ^ 2 + ‖Dtw z‖ₑ ^ 2 < ⊤)
:
∫⁻ (z : CKN.Foundation.Parabolic.ParabolicPoint) in ucCylinder ρ, ‖ucScaledField x₀ scale w z‖ₑ ^ 2 + ‖ucScaledDw x₀ scale Dw z‖ₑ ^ 2 + ‖ucScaledD2w x₀ scale D2w z‖ₑ ^ 2 + ‖ucScaledDtw x₀ scale Dtw z‖ₑ ^ 2 < ⊤
Finite quadratic weak-derivative data transfers to the normalized Gaussian cylinder.