Homogeneous material derivatives from actual analytic scalar energies.
theorem
AVenhance.Infra.Section4.iterate_analytic_homogeneous_material_energy_bound
{b : ℝ → Homogenization.Vec 2 → Homogenization.Vec 2}
{κ : ℝ}
{u : ℝ → Homogenization.Vec 2 → ℝ}
{u₀ : Homogenization.Vec 2 → ℝ}
(hsol : IsClassicalSol b κ (fun (x : ℝ) (x_1 : Homogenization.Vec 2) => 0) u₀ u)
(hb : ContDiffOn ℝ (↑⊤) (fun (z : AmnrSpace) => b z.1 z.2) (Set.Ici 0 ×ˢ Set.univ))
(w : List (Fin 2))
(a : ℕ)
{B G r L C : ℝ}
(hB : 0 ≤ B)
(hr : 0 ≤ r)
(hC : 0 ≤ C)
(hκ : 0 < κ)
(hL : 0 < L)
(hg : 2 * (r / L) ^ 2 ≤ 1 / 2)
(hscale : B * r ≤ C * κ * L ^ 2)
(hjet :
∀ (t : ℝ) (x : Homogenization.Vec 2),
∀ p ∈ List.filter (fun (p : List (Fin 2) × List (Fin 2)) => decide (1 ≤ p.1.length)) (iterateSpatialSplits w),
∀ (j : Fin 2),
|iterateSpatialWord p.1 (fun (y : Homogenization.Vec 2) => b t y j) x| ≤ B * ↑p.1.length.factorial * r ^ p.1.length)
(hE :
∀ (q : List (Fin 2)),
q.length ≤ w.length + 1 →
(spaceTimeGradNormSq fun (t : ℝ) => spaceGrad (iterateSpatialWord q (u t))) ≤ G ^ 2 * (↑(q.length + a).factorial * L ^ q.length) ^ 2)
:
The actual homogeneous PDE bounds each material word using only actual one-higher scalar gradients and velocity jets. No material bound is assumed.