Derivatives on the Gaussian cutoff plateau #
The spatial factor is constant on the inner ball, and both time factors are constant away from their transition intervals.
theorem
ESS.ucSpatialCutoff_spatialPartial_zero_on_inner
{ρ : ℝ}
(hρ : 0 < ρ)
{x : CKN.Foundation.Parabolic.Vec3}
(hx : x ∈ CKN.Foundation.Parabolic.vec3Ball 0 (ρ / 2))
(j : Fin 3)
(s : ℝ)
:
CKN.spatialPartial (fun (q : CKN.Foundation.Parabolic.ParabolicPoint) => ucSpatialCutoff ρ hρ q.1) j (x, s) = 0
The first spatial derivative of the ball cutoff vanishes on its inner plateau.
theorem
ESS.ucSpatialCutoff_spatialSecondPartial_zero_on_inner
{ρ : ℝ}
(hρ : 0 < ρ)
{x : CKN.Foundation.Parabolic.Vec3}
(hx : x ∈ CKN.Foundation.Parabolic.vec3Ball 0 (ρ / 2))
(j k : Fin 3)
(s : ℝ)
:
CKN.spatialSecondPartial (fun (q : CKN.Foundation.Parabolic.ParabolicPoint) => ucSpatialCutoff ρ hρ q.1) j k (x, s) = 0
The second spatial derivative of the ball cutoff vanishes on its inner plateau.
theorem
ESS.ucGaussianCutoff_spatialPartial_zero_on_inner
{ρ : ℝ}
(hρ : 0 < ρ)
(ε : ℝ)
{z : CKN.Foundation.Parabolic.ParabolicPoint}
(hz : z ∈ ucInnerRegion ρ)
(j : Fin 3)
:
The Gaussian cutoff has no first spatial derivative on the inner ball.
theorem
ESS.ucGaussianCutoff_spatialSecondPartial_zero_on_inner
{ρ : ℝ}
(hρ : 0 < ρ)
(ε : ℝ)
{z : CKN.Foundation.Parabolic.ParabolicPoint}
(hz : z ∈ ucInnerRegion ρ)
(j k : Fin 3)
:
The Gaussian cutoff has no second spatial derivative on the inner ball.
The final-time factor has zero derivative before its transition.
The initial-time factor has zero derivative after its transition.
theorem
ESS.ucGaussianCutoff_timePartial_zero_on_inner_late
{ρ ε : ℝ}
(hρ : 0 < ρ)
(hε : 0 < ε)
{z : CKN.Foundation.Parabolic.ParabolicPoint}
(hz : z ∈ ucInnerRegion ρ)
(hlate : 2 * ε < z.2)
:
Away from the initial transition, the Gaussian cutoff has zero time derivative on the inner region.