Heat operator on the Gaussian cutoff plateau #
All cutoff derivatives vanish in the interior after the initial time transition, leaving the original weak heat operator.
theorem
ESS.ucGaussianCutoff_heat_eq_on_inner
{ρ : ℝ}
(hρ : 0 < ρ)
(ε : ℝ)
{z : CKN.Foundation.Parabolic.ParabolicPoint}
(hz : z ∈ ucInnerRegion ρ)
(v : 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)
:
ucCutoffHeat (ucSpatialCutoff ρ hρ) ucFinalTimeCutoff (ucInitialTimeCutoff ε) v Dw D2w Dtw z = ucInitialTimeCutoff ε z.2 • ucWeakHeatVector D2w Dtw z + deriv (ucInitialTimeCutoff ε) z.2 • v z
On the inner region, the only cutoff error comes from the initial time transition.
theorem
ESS.ucGaussianCutoff_field_eq_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)
(v : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
:
The compact field equals the original field on the late interior.
theorem
ESS.ucGaussianCutoff_dw_eq_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)
(v : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Dv : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
:
The first weak derivative data agree on the late interior.
The initial cutoff derivative vanishes before its transition.