Stream-regularity coefficient bounds in the first-derivative drift estimate.
theorem
AVenhance.Infra.Section4.iterate_stream_word_factorial_bound_of_A3
{β : ℝ}
(I : Ingredients β)
{Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ}
(hΦ : IsStreamSeq I Φ)
{m : ℕ}
(hm : 2 ≤ m)
(hA3 :
∀ (j : ℕ),
1 ≤ j →
∀ (t : ℝ) (n : ℕ),
2 ≤ n →
barNorm n (2 ^ 8 * (epsilon β I.Λ j)⁻¹) (Φ j t) ≤ ENNReal.ofReal (2 ^ 5 * AVenhance.a β I.Λ j * epsilon β I.Λ j ^ 2 * ((↑n + 2) ^ 2 / (↑n + 1) ^ 3)))
(t : ℝ)
(w : List (Fin 2))
(hw : 2 ≤ w.length)
(x : Homogenization.Vec 2)
:
All high spatial stream jets obey the source factorial profile under the stream-regularity premise. This is the coefficient profile used in the drift sum.
theorem
AVenhance.Infra.Section4.iterate_stream_second_jet_bound_of_A3
{β : ℝ}
(I : Ingredients β)
{Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ}
(hΦ : IsStreamSeq I Φ)
{m : ℕ}
(hm : 2 ≤ m)
(hA3 :
∀ (j : ℕ),
1 ≤ j →
∀ (t : ℝ) (n : ℕ),
2 ≤ n →
barNorm n (2 ^ 8 * (epsilon β I.Λ j)⁻¹) (Φ j t) ≤ ENNReal.ofReal (2 ^ 5 * AVenhance.a β I.Λ j * epsilon β I.Λ j ^ 2 * ((↑n + 2) ^ 2 / (↑n + 1) ^ 3)))
(t : ℝ)
(x : Homogenization.Vec 2)
(i j : Fin 2)
:
The Hessian entries needed by the first-derivative drift error have a fixed numerical bound times the physical stream-amplitude scale.
theorem
AVenhance.Infra.Section4.iterate_velocity_word_bound_of_A3
{β : ℝ}
(I : Ingredients β)
{Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ}
(hΦ : IsStreamSeq I Φ)
{m : ℕ}
(hm : 2 ≤ m)
(hA3 :
∀ (j : ℕ),
1 ≤ j →
∀ (t : ℝ) (n : ℕ),
2 ≤ n →
barNorm n (2 ^ 8 * (epsilon β I.Λ j)⁻¹) (Φ j t) ≤ ENNReal.ofReal (2 ^ 5 * AVenhance.a β I.Λ j * epsilon β I.Λ j ^ 2 * ((↑n + 2) ^ 2 / (↑n + 1) ^ 3)))
(t : ℝ)
(w : List (Fin 2))
(hw : 1 ≤ w.length)
(x : Homogenization.Vec 2)
(i : Fin 2)
:
The stream-regularity estimates also control every positive-order velocity jet appearing in the material oscillatory errors. The component formula and derivative commutation are proved from the stream velocity.