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LeanPool.AnomalousDiffusion.AVenhance.Infra.Section5.Contracts.TermCenteredNormie3Analytic

Composed analyticity of the slow factor of normie3 #

n3Slow_{pj} = slowFactorChoice3 ξ_k Y F (T t) p j with Y = Fᵀ (the transpose of the flow Jacobian, not 1 - Fᵀ), so the choice-3 composed bound of SlowFactorBoundsComposition applies with the word bound 41 of the entries of Q = F (sdj_Q_word).

theorem AVenhance.Infra.Section5.Contracts.n3Slow_eq_choice3 {β : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) (m : ℕ) (T : ℝ → Homogenization.Vec 2 → ℝ) (k : ℤ) (t : ℝ) (hT : ContDiff ℝ (↑⊤) (T t)) (p j : Fin 2) :
n3Slow I hΦ m T k t p j = slowFactorChoice3 (I.xiMK m k t) (fun (x : Homogenization.Vec 2) => (I.flowGrad hΦ m (lIdx β I.Λ m k) t x).transpose) (I.flowGrad hΦ m (lIdx β I.Λ m k) t) (T t) p j
theorem AVenhance.Infra.Section5.Contracts.n3c_core {β : ℝ} (A : ℝ) (hA : 1 ≤ A) {K : ℝ} (hK1 : 1 ≤ K) (hK : ∀ (n : ℕ), (↑n + 3) ^ 5 ≤ K * 2 ^ n) (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) {m : ℕ} (hm : 2 ≤ m) {S : ℝ} (hS : 0 ≤ S) (T : ℝ → Homogenization.Vec 2 → ℝ) (hJets : RelativeError.PositiveTemperatureJets A (epsilon β I.Λ (m - 1) ^ (1 + gamma β / 2)) S T) (hTs : ∀ (t : ℝ), 0 ≤ t → ContDiff ℝ (↑⊤) (T t)) (hTp : ∀ (t : ℝ), 0 ≤ t → IsZ2Periodic (T t)) {t : ℝ} (ht : t ∈ Set.Ioo 0 1) {k : ℤ} (hξ : I.xiMK m k t ≠ 0) (p j : Fin 2) :
Ergodic.HasCoordinateAnalyticL2Bounds (fun (x : Homogenization.Vec 2) => ↑(n3Slow I hΦ m T k t p j (I.xFlow hΦ m (lIdx β I.Λ m k) t x))) (64 * 41 * 41 * A * max A (2 ^ 14) ^ 2 * S * ((epsilon β I.Λ (m - 1) ^ (1 + gamma β / 2)) ^ 2)⁻¹) (epsilon β I.Λ (m - 1) ^ (1 + gamma β / 2) / (2 * 2 ^ 14 * 33 * K * max A (2 ^ 14)))

The core of n3_slow_composed_bounds, with the constants explicit. Here A₁ = max A 2^14, K is the absolute polynomial-versus-exponential constant.

theorem AVenhance.Infra.Section5.Contracts.n3_slow_composed_bounds (β A : ℝ) (hA : 1 ≤ A) :
∃ (c₁ : ℝ) (c₂ : ℝ), 0 < c₁ ∧ 0 < c₂ ∧ ∀ (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) {m : ℕ}, 2 ≤ m → ∀ {S : ℝ}, 0 ≤ S → ∀ (T : ℝ → Homogenization.Vec 2 → ℝ), RelativeError.PositiveTemperatureJets A (epsilon β I.Λ (m - 1) ^ (1 + gamma β / 2)) S T → (∀ (t : ℝ), 0 ≤ t → ContDiff ℝ (↑⊤) (T t)) → (∀ (t : ℝ), 0 ≤ t → IsZ2Periodic (T t)) → epsilon β I.Λ (m - 1) ^ (2 * delta β) ≤ 1 / 4 → ∀ {t : ℝ}, t ∈ Set.Ioo 0 1 → ∀ {k : ℤ}, I.xiMK m k t ≠ 0 → ∀ (p j : Fin 2), Ergodic.HasCoordinateAnalyticL2Bounds (fun (x : Homogenization.Vec 2) => ↑(n3Slow I hΦ m T k t p j (I.xFlow hΦ m (lIdx β I.Λ m k) t x))) (c₁ * S * ((epsilon β I.Λ (m - 1) ^ (1 + gamma β / 2)) ^ 2)⁻¹) (epsilon β I.Λ (m - 1) ^ (1 + gamma β / 2) / c₂)

Composed analyticity of the slow factor of normie3 on supp ξ_{m,k}. The constants depend only on the jet constant A and β.