Plateau of the short-time cutoff #
In the spatial interior, after the lower-time transition, and above the phase gap, the compact cutoff is locally constant one.
The open plateau of the full compact cutoff.
Equations
- ESS.buShortCoreRegion scale R ε = {q : CKN.Foundation.Parabolic.Vec3 × ℝ | q.1 ∈ CKN.Foundation.Parabolic.vec3Ball 0 R ∧ q ∈ ESS.buShortAboveGap scale ∧ 1 / 2 + 2 * ε < q.2}
Instances For
The cutoff plateau is open.
theorem
ESS.buShortFullCutoff_eq_one_on_core
(scale R ε : ℝ)
(hscale : 0 < scale)
(hscale1 : scale ≤ 1)
(hR : 0 < R)
(hε : 0 < ε)
:
Set.EqOn (buShortFullCutoff scale R hR ε) (fun (x : CKN.Foundation.Parabolic.Vec3 × ℝ) => 1)
(buShortCoreRegion scale R ε)
All three cutoff factors equal one on the plateau.
theorem
ESS.buShortFullCutoff_derivatives_zero_on_core
(scale R ε : ℝ)
(hscale : 0 < scale)
(hscale1 : scale ≤ 1)
(hR : 0 < R)
(hε : 0 < ε)
{z : CKN.Foundation.Parabolic.ParabolicPoint}
(hz : CKN.Foundation.Parabolic.parabolicHomeomorph z ∈ buShortCoreRegion scale R ε)
:
(∀ (j : Fin 3), CKN.spatialPartial (buCutScalar (buShortFullCutoff scale R hR ε)) j z = 0) ∧ (∀ (j k : Fin 3), CKN.spatialSecondPartial (buCutScalar (buShortFullCutoff scale R hR ε)) j k z = 0) ∧ CKN.timePartial (buCutScalar (buShortFullCutoff scale R hR ε)) z = 0
The first, second, and time derivatives of the full cutoff vanish throughout its open plateau.