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LeanPool.EscauriazaSereginSverak.Endpoint.EssLocalInteriorUC

Unique continuation at a translated top time #

The unique continuation theorem thm:uc is stated at the spatial origin and initial time zero of a forward cylinder. Reversing time about a top time t₀ and translating the spatial center to x₀ transports it to past cylinders B_R(x₀) × (t₀ - T, t₀]. Vanishing on a small past cylinder at the top point gives the infinite-order hypothesis by lem:flat-from-vanishing.

theorem ESS.essLocal_uniqueContinuation_past (R T C M r₀ : ℝ) (hR : 0 < R) (hT : 0 < T) (hC : 0 ≤ C) (hM : 0 ≤ M) (hr₀ : 0 < r₀) (hr₀R : r₀ ≤ R) (hr₀T : r₀ ^ 2 ≤ T) (x₀ : CKN.Foundation.Parabolic.Vec3) (t₀ : ℝ) (ω : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3) (Dω : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3) (D2ω : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3) (Dtω : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3) (hcont : ContinuousOn ω (CKN.spaceTimeSet (CKN.Foundation.Parabolic.vec3Ball x₀ R) (Set.Ioc (t₀ - T) t₀))) (hderiv : CKN.HasSpaceTimeWeakDerivs (CKN.Foundation.Parabolic.vec3Ball x₀ R) (Set.Ioo (t₀ - T) t₀) ω Dω D2ω Dtω) (hL2 : ∫⁻ (z : CKN.Foundation.Parabolic.ParabolicPoint) in CKN.spaceTimeSet (CKN.Foundation.Parabolic.vec3Ball x₀ R) (Set.Ioo (t₀ - T) t₀), ‖ω z‖ₑ ^ 2 + ‖Dω z‖ₑ ^ 2 + ‖D2ω z‖ₑ ^ 2 + ‖Dtω z‖ₑ ^ 2 < ⊤) (hineq : ∀ᵐ (z : CKN.Foundation.Parabolic.ParabolicPoint) ∂MeasureTheory.volume.restrict (CKN.spaceTimeSet (CKN.Foundation.Parabolic.vec3Ball x₀ R) (Set.Ioo (t₀ - T) t₀)), (CKN.Foundation.Parabolic.vec3EuclideanNorm fun (i : Fin 3) => Dtω z i - ∑ j : Fin 3, D2ω z i j j) ≤ C * (CKN.Foundation.Parabolic.vec3EuclideanNorm (ω z) + √(CKN.spatialGradientSq ω Dω z))) (hbound : ∀ z ∈ CKN.spaceTimeSet (CKN.Foundation.Parabolic.vec3Ball x₀ R) (Set.Ioc (t₀ - T) t₀), CKN.Foundation.Parabolic.vec3EuclideanNorm (ω z) ≤ M) (hzero : ∀ (x : CKN.Foundation.Parabolic.Vec3) (s : ℝ), x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ r₀ → s ∈ Set.Ioo (t₀ - r₀ ^ 2) t₀ → ω (x, s) = 0) (x : CKN.Foundation.Parabolic.Vec3) :
x ∈ CKN.Foundation.Parabolic.vec3Ball x₀ R → ω (x, t₀) = 0

Unique continuation for the backward heat inequality on a past cylinder: a bounded continuous field of class W^{2,1}_2 satisfying |∂ₜω - Δω| ≤ C (|ω| + |∇ω|) which vanishes on a small past cylinder at the top point (x₀, t₀) vanishes on the whole top ball (thm:uc, lem:flat-from-vanishing).