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LeanPool.EscauriazaSereginSverak.Linear.BUShortCoreEstimate

Quantitative mass bound in the positive-phase plateau #

The absorbed half-space estimate and the global cutoff error bound control every fixed measurable part of the cutoff plateau.

theorem ESS.bu_short_core_mass_bound :
∃ (a₀ : ℝ) (c : ℝ), 0 < a₀ ∧ 0 < c ∧ ∀ (scale R ε c₁ C₁ C₂ a : ℝ), 0 < scale → scale ≤ 1 → ∀ (hR : 1 ≤ R), 0 < ε → 0 ≤ c₁ → 0 ≤ C₁ → (∀ (scale y : ℝ), |deriv (deriv (buShortNormalCutoff scale)) y| ≤ C₁) → 0 ≤ C₂ → (∀ (x : ℝ), |deriv (deriv CKN.smoothTransitionProfile) x| ≤ C₂) → c * 36 * (c₁ * scale) ^ 2 ≤ 1 / 2 → max a₀ 1 < a → ∀ (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), ContinuousOn w ({x : CKN.Foundation.Parabolic.Vec3 | 0 < x 2} ×ˢ Set.Ico 0 1) → CKN.HasSpaceTimeWeakDerivs {x : CKN.Foundation.Parabolic.Vec3 | 0 < x 2} (Set.Ioo 0 1) w Dw D2w Dtw → (∀ 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 < ⊤) → (∀ᵐ (z : CKN.Foundation.Parabolic.ParabolicPoint) ∂MeasureTheory.volume.restrict (CKN.spaceTimeSet {x : CKN.Foundation.Parabolic.Vec3 | 0 < x 2} (Set.Ioo 0 1)), CKN.Foundation.Parabolic.vec3EuclideanNorm (ucWeakHeatVector D2w Dtw z) ≤ c₁ * (√(CKN.spatialGradientSq w Dw z) + CKN.Foundation.Parabolic.vec3EuclideanNorm (w z))) → MeasureTheory.IntegrableOn (fun (z : CKN.Foundation.Parabolic.ParabolicPoint) => Real.exp (-(z.1 0 ^ 2 + z.1 1 ^ 2) / (4 * z.2)) * (1 + z.1 2) ^ 4 * (CKN.Foundation.Parabolic.vec3EuclideanNorm (buAffineField (-scale ^ 2 / 2) scale w z) ^ 2 + CKN.spatialGradientSq (buAffineField (-scale ^ 2 / 2) scale w) (buAffineDw (-scale ^ 2 / 2) scale Dw) z)) (buShortWideGapRegion scale) MeasureTheory.volume → MeasureTheory.IntegrableOn (fun (z : CKN.Foundation.Parabolic.ParabolicPoint) => buShortShiftedWeight scale a z * (1 + z.1 2) ^ 4 * (CKN.Foundation.Parabolic.vec3EuclideanNorm (buAffineField (-scale ^ 2 / 2) scale w z) ^ 2 + CKN.spatialGradientSq (buAffineField (-scale ^ 2 / 2) scale w) (buAffineDw (-scale ^ 2 / 2) scale Dw) z)) (buShortHighStrip scale) MeasureTheory.volume → MeasureTheory.IntegrableOn (fun (z : CKN.Foundation.Parabolic.ParabolicPoint) => buShortShiftedWeight scale a z * (CKN.Foundation.Parabolic.vec3EuclideanNorm (buAffineField (-scale ^ 2 / 2) scale w z) ^ 2 + CKN.spatialGradientSq (buAffineField (-scale ^ 2 / 2) scale w) (buAffineDw (-scale ^ 2 / 2) scale Dw) z)) (buShortHighStrip scale) MeasureTheory.volume → ∀ (S : Set CKN.Foundation.Parabolic.ParabolicPoint), MeasurableSet S → (∀ z ∈ S, CKN.Foundation.Parabolic.parabolicHomeomorph z ∈ buShortCoreRegion scale R ε) → have K := buCutSupportSet (buShortFullCutoff scale R ⋯ ε); have v := buAffineField (-scale ^ 2 / 2) scale w; have Dv := buAffineDw (-scale ^ 2 / 2) scale Dw; ∫ (z : CKN.Foundation.Parabolic.ParabolicPoint) in S, buShortShiftedWeight scale a z * CKN.Foundation.Parabolic.vec3EuclideanNorm (v z) ^ 2 ≤ 4 * c * (((4 * buShortUniformErrorCoeff scale c₁ C₁ C₂ ^ 2 * Real.exp (-(a * buShortD scale)) * ∫ (z : CKN.Foundation.Parabolic.ParabolicPoint) in buShortWideGapRegion scale, Real.exp (-(z.1 0 ^ 2 + z.1 1 ^ 2) / (4 * z.2)) * (1 + z.1 2) ^ 4 * (CKN.Foundation.Parabolic.vec3EuclideanNorm (v z) ^ 2 + CKN.spatialGradientSq v Dv z)) + 4 * buShortShellCoeff scale R c₁ ^ 2 * ∫ (z : CKN.Foundation.Parabolic.ParabolicPoint) in buShortHighStrip scale, buShortShiftedWeight scale a z * (CKN.Foundation.Parabolic.vec3EuclideanNorm (v z) ^ 2 + CKN.spatialGradientSq v Dv z)) + 2 * ∫ (z : CKN.Foundation.Parabolic.ParabolicPoint) in K, 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)

The mass on a fixed cutoff plateau is controlled by the negative phase gap, spatial shell, and lower-time transition.