Integrable lower-time transition density

At fixed radius and transition width, the shifted Carleman density times the time-supported quadratic field belongs to L¹.

theorem ESS.bu_short_shifted_early_integrable (scale R ε a : ℝ) (hscale : 0 < scale) (hscale1 : scale ≤ 1) (hR : 0 < R) (hε : 0 < ε) (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) (hcont : ContinuousOn w ({x : CKN.Foundation.Parabolic.Vec3 | 0 < x 2} ×ˢ Set.Ico 0 1)) (hweak : CKN.HasSpaceTimeWeakDerivs {x : CKN.Foundation.Parabolic.Vec3 | 0 < x 2} (Set.Ioo 0 1) w Dw D2w Dtw) (hL2 : ∀ S ⊆ CKN.spaceTimeSet {x : CKN.Foundation.Parabolic.Vec3 | 0 < x 2} (Set.Ioo 0 1), Bornology.IsBounded S → ∫⁻ (z : CKN.Foundation.Parabolic.ParabolicPoint) in S, ‖Dw z‖ₑ ^ 2 + ‖D2w z‖ₑ ^ 2 + ‖Dtw z‖ₑ ^ 2 < ⊤) : have K := buCutSupportSet (buShortFullCutoff scale R hR ε); have v := buAffineField (-scale ^ 2 / 2) scale w; MeasureTheory.IntegrableOn (fun (z : CKN.Foundation.Parabolic.ParabolicPoint) => buShortShiftedWeight scale a z * (if 1 / 2 + ε ≤ z.2 ∧ z.2 ≤ 1 / 2 + 2 * ε then 8 / ε * CKN.Foundation.Parabolic.vec3EuclideanNorm (v z) else 0) ^ 2) K MeasureTheory.volume

The shifted lower-time transition density is integrable on the compact cutoff support.