Iterates Homogeneous Previous Material #
Support for the Armstrong–Vicol anomalous-diffusion formalization.
theorem
AVenhance.Infra.Section4.iterate_homogeneous_terminal_previous_material_squared_gain
{b : ℝ → Homogenization.Vec 2 → Homogenization.Vec 2}
{κ : ℝ}
{u v : ℝ → Homogenization.Vec 2 → ℝ}
{v₀ : Homogenization.Vec 2 → ℝ}
(hsol : IsClassicalSol b κ (fun (x : ℝ) (x_1 : Homogenization.Vec 2) => 0) v₀ v)
(hb : ContDiffOn ℝ (↑⊤) (fun (z : AmnrSpace) => b z.1 z.2) (Set.Ici 0 ×ˢ Set.univ))
(hu : ContDiffOn ℝ (↑⊤) (fun (z : AmnrSpace) => u z.1 z.2) (Set.Ici 0 ×ˢ Set.univ))
(w : List (Fin 2))
{Q : ℝ → Matrix (Fin 2) (Fin 2) ℝ}
(hQc : ContinuousOn (fun (z : AmnrSpace) => Q z.1) (Set.Ici 0 ×ˢ Set.univ))
{B N r L Cv Cs D q s : ℝ}
(hB : 0 ≤ B)
(hr : 0 ≤ r)
(hCv : 0 ≤ Cv)
(hκ : 0 < κ)
(hL : 0 < L)
(hg : 2 * (r / L) ^ 2 ≤ 1 / 2)
(hvelocity : B * r ≤ Cv * κ * L ^ 2)
(hjet :
∀ (t : ℝ) (x : Homogenization.Vec 2) (p : List (Fin 2)),
1 ≤ p.length →
∀ (j : Fin 2),
|iterateSpatialWord p (fun (y : Homogenization.Vec 2) => b t y j) x| ≤ B * ↑p.length.factorial * r ^ p.length)
(hE :
∀ (p : List (Fin 2)),
p.length ≤ w.length + 2 →
(spaceTimeGradNormSq fun (t : ℝ) => spaceGrad (iterateSpatialWord p (v t))) ≤ (N / √κ) ^ 2 * (↑p.length.factorial * L ^ p.length) ^ 2)
(hD : 0 ≤ D)
(hCs : 0 ≤ Cs)
(hq : 0 ≤ q)
(hQ : ∀ (t : ℝ) (j k : Fin 2), |Q t j k| ≤ D)
(hscale : D * L ^ 2 ≤ Cs * q)
(hs1 : s ≤ 1)
:
|∫ (z : AmnrSpace) in iterateTruncatedCell s, Homogenization.vecDot (spaceGrad (iterateSpatialWord w (u z.1)) z.2)
((Q z.1).mulVec (spaceGrad (amnrMaterial b (fun (t : ℝ) => iterateSpatialWord w (v t)) z.1) z.2))| ≤ (κ / 24 * spaceTimeGradNormSq fun (t : ℝ) => spaceGrad (iterateSpatialWord w (u t))) + 24 * Cs ^ 2 * (8 + 544 * Cv ^ 2) * q ^ 2 * N ^ 2 * (↑(w.length + 2).factorial * L ^ w.length) ^ 2
The actual homogeneous PDE supplies the exceptional first previous-material term at q squared from conditional scalar analytic energies.