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LeanPool.AnomalousDiffusion.AVenhance.Infra.Section4.IteratesActualTerminalCurrent

Actual current increment with the corrected material budget.

theorem AVenhance.Infra.Section4.iterate_increment_terminal_current_material_corrected_bound {β : ℝ} (I : Ingredients β) {Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hΦ : IsStreamSeq I Φ) {m : ℕ} {κm κprev : ℝ} {θ₀ : Homogenization.Vec 2 → ℝ} {θprev : ℝ → Homogenization.Vec 2 → ℝ} {T : ℕ → ℝ → Homogenization.Vec 2 → ℝ} (hT : I.IsTIterates hΦ m κm κprev θ₀ θprev T) (hθ : IsClassicalSol (streamVel (Φ (m - 1))) κprev (fun (x : ℝ) (x_1 : Homogenization.Vec 2) => 0) θ₀ θprev) (hm : 1 ≤ m) (hκm : 0 < κm) (hκ : 0 < κprev) (hflow : ∀ (l : ℤ), ContDiff ℝ ↑⊤ fun (z : AmnrSpace) => I.flowGrad hΦ m l z.1 z.2) {s : ℝ} (hs1 : s ≤ 1) (i : ℕ) (hi : i + 1 ≤ Nstar β) (w : List (Fin 2)) {Ccoef Cscale B r L D q : ℝ} (hL : 0 < L) (hg : 2 * (r / L) ^ 2 ≤ 1 / 2) (hD : 0 ≤ D) (hCscale : 0 ≤ Cscale) (hq : 0 < q) {Q : ℝ → Matrix (Fin 2) (Fin 2) ℝ} (hQc : ContinuousOn Q (Set.Ici 0)) (hQ : ∀ (t : ℝ) (j k : Fin 2), |Q t j k| ≤ D) (hscale : D * L ^ 2 ≤ Cscale * q) (hcoef : ∀ (t : ℝ) (x : Homogenization.Vec 2) (p : List (Fin 2)) (j k : Fin 2), |iterateMatrixWord (fun (y : Homogenization.Vec 2) => I.Kmat κm m t - κprev • 1 + I.sMat hΦ m κm t y) p x j k| ≤ κprev * Ccoef * ↑p.length.factorial * r ^ p.length) (hprev : ∀ (p : List (Fin 2)), p.length ≤ w.length + 2 → (spaceTimeGradNormSq fun (t : ℝ) => spaceGrad (iterateSpatialWord p (iterateIncrement T i t))) ≤ B ^ 2 * (↑(p.length + 2 * i).factorial * L ^ p.length) ^ 2) :
|∫ (z : AmnrSpace) in iterateTruncatedCell s, Homogenization.vecDot (spaceGrad (iterateSpatialWord w (amnrMaterial (streamVel (Φ (m - 1))) (iterateIncrement T (i + 1)) z.1)) z.2) ((Q z.1).mulVec (spaceGrad (iterateSpatialWord w (iterateIncrement T i z.1)) z.2))| ≤ (κprev / 24 * spaceTimeGradNormSq fun (t : ℝ) => spaceGrad (iterateSpatialWord w (iterateIncrement T (i + 1) t))) + (24 * Cscale ^ 2 * q ^ 2 + (1 + Cscale ^ 2 * (32 * Ccoef ^ 2)) * q) * (4 * κprev * B ^ 2 * (↑(w.length + 2 + 2 * i).factorial * L ^ w.length) ^ 2)

Derive the linear and quadratic oscillatory remainder from actual forcing jets and the preceding increment energies.