Positive-order temperature jets and arbitrary amplitude; no zeroth-order temperature supremum. Existing Sobolev, product and composition engines are reused.
theorem
AVenhance.Infra.Section5.RelativeError.orderedPartial_comp_le
{K : ℝ}
(hK1 : 1 ≤ K)
(hK : ∀ (n : ℕ), (↑n + 3) ^ 5 ≤ K * 2 ^ n)
{A ρ e N : ℝ}
(hA : 1 ≤ A)
(hρ : 0 < ρ)
(hρe : ρ ≤ e)
(he1 : e ≤ 1)
(hN : 0 < N)
{f : Homogenization.Vec 2 → ℝ}
(hf : ContDiff ℝ (↑⊤) f)
(hp : IsZ2Periodic f)
(hreg :
∀ (n : ℕ) (i : Fin n → Fin 2),
0 < n →
√(l2NormSq fun (x : Homogenization.Vec 2) =>
(iteratedFDeriv ℝ n f x) fun (j : Fin n) => Homogenization.basisVec (i j)) ≤ A * N * ↑n.factorial * (A / ρ) ^ n)
{X : Homogenization.Vec 2 → Homogenization.Vec 2}
(hX : AnalyticBridge.FlowForErgodicBound A e X)
(hXs : ContDiff ℝ (↑⊤) X)
(i j : Fin 2)
(n : ℕ)
(x : Homogenization.Vec 2)
(I : Fin n → Fin 2)
:
‖FaaDiBruno.orderedPartial n
((fun (y : Homogenization.Vec 2) =>
(fderiv ℝ f y) (Homogenization.basisVec i) * (fderiv ℝ f y) (Homogenization.basisVec j)) ∘ X)
x I‖ ≤ 4 * (3 * AnalyticBridge.sobolevConst * (A * N) * K * (A / ρ) ^ 3) ^ 2 * ↑n.factorial * (2 * A / e * (1 + ↑2 * (K * e) * (2 * (A / ρ)))) ^ n
Pointwise bound on the ordered partials of (∂_i f ∂_j f) ∘ X.