base energy at the later start("The coarse diffusivity satisfies ...", #
"Poincaré at 9166–9190 gives ...") and §6 item 11. For j = laterStart β Λ R < M:
κ_j ≥ c R^{p₊}(from the diffusivity lower boundκ_j ≥ c₀ ε_j^{β+γ}, the minimality ofj, and, forj = 1, the radius boundR ≤ 1/(√2 π));κ_j ‖∇θ_j‖² ≥ c R^{p₊} ‖g‖²from the energy identity and Poincaré.
The κ conjunct is stated for nonzero data (0 < l2NormSq g →): for g = 0 and large R the
index j = 1 is the later start while R^{p₊} is unbounded, so it cannot hold uniformly.
theorem
AVenhance.Infra.Section5.RelativeError.kappa_lower_of_cases
{c₀ e₁ p R Kj eJ : ℝ}
{j : ℕ}
(hc₀ : 0 < c₀)
(he₁ : 0 < e₁)
(hp : 0 < p)
(hR : 0 < R)
{h : ℝ}
(hKj : c₀ * eJ ≤ Kj)
(hj1 : j = 1 → eJ = e₁)
(hj2 : 2 ≤ j → (1 / 2) ^ h * R ^ p ≤ eJ)
(hj0 : 1 ≤ j)
(hR1 : j = 1 → R ≤ 1)
:
The abstract lower bound for κ_j at the later start, in terms of a constant c₁.
theorem
AVenhance.Infra.Section5.RelativeError.later_base_energy
(β C₀ : ℝ)
(hβ : 6 / 5 ≤ β)
(Λ : ℕ)
:
2 ^ 7 ≤ Λ →
∃ (c : ℝ),
0 < c ∧ ∀ (I : Ingredients β),
I.Λ = Λ →
I.Czeta ≤ C₀ →
I.Cxi ≤ C₀ →
I.Chat ≤ C₀ →
∀ (Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ),
IsStreamSeq I Φ →
∀ κ ∈ permissibleSet β I.Λ,
∀ (M : ℕ),
1 ≤ M →
κ ∈ permittedInterval β I.Λ M →
∀ (R : ℝ),
0 < R →
laterStart β I.Λ R < M →
∀ (g : Homogenization.Vec 2 → ℝ),
ContDiff ℝ (↑⊤) g →
IsZ2Periodic g →
Homogenization.MeanZeroOn unitCube g →
IsThetaAnalytic R g →
∀ (θ : ℝ → Homogenization.Vec 2 → ℝ),
IsClassicalSol (streamVel (Φ (laterStart β I.Λ R)))
(I.kappaSeq κ M (laterStart β I.Λ R))
(fun (x : ℝ) (x_1 : Homogenization.Vec 2) => 0) g θ →
(0 < l2NormSq g →
c * R ^ pPlus β ≤ I.kappaSeq κ M (laterStart β I.Λ R)) ∧ c * R ^ pPlus β * l2NormSq g ≤ I.kappaSeq κ M (laterStart β I.Λ R) * spaceTimeGradNormSq fun (t : ℝ) (x : Homogenization.Vec 2) =>
spaceGrad (θ t) x
Item 11: base energy at the later start, with c after β, C₀, Λ and before κ, M, R, g.
The κ conjunct is for nonzero data (see the module docstring).