Joint continuity of the leading matrix F #
Source: enhance.tex 8298–8302. Near each time only finitely many modes ξ_{m,k} are active
(their supports have length (5/2)τ_m), so F is locally a finite sum of jointly continuous
matrix fields ξ_{m,k}(t) (I + ∇Χ_{m,k}(t,·)) ∘ X⁻¹_{m-1,l_k}(t,x).
theorem
AVenhance.Infra.Section5.LeftToShow.continuous_gradMatrix_chiMK
{β : ℝ}
(I : Ingredients β)
(κ : ℝ)
(m : ℕ)
{k : ℤ}
(hk : Odd k)
:
Continuous fun (q : ℝ × Homogenization.Vec 2) => gradMatrix (I.chiMK κ m k q.1) q.2
A single mode's corrector gradient is jointly continuous in time and position.
theorem
AVenhance.Infra.Section5.LeftToShow.continuous_xiMK
{β : ℝ}
(I : Ingredients β)
(m : ℕ)
(k : ℤ)
:
Continuous (I.xiMK m k)
noncomputable def
AVenhance.Infra.Section5.LeftToShow.leadingSummand
{β : ℝ}
(I : Ingredients β)
{Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ}
(hΦ : IsStreamSeq I Φ)
(m : ℕ)
(κm : ℝ)
(k : ℤ)
(q : ℝ × Homogenization.Vec 2)
:
The k-th summand of F, as a function of the spacetime point.
Equations
- AVenhance.Infra.Section5.LeftToShow.leadingSummand I hΦ m κm k q = I.xiMK m k q.1 • (1 + AVenhance.gradMatrix (I.chiMK κm m k q.1) (I.xFlowInv hΦ m (AVenhance.lIdx β I.Λ m k) q.1 q.2))
Instances For
theorem
AVenhance.Infra.Section5.LeftToShow.continuous_leadingSummand
{β : ℝ}
(I : Ingredients β)
{Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ}
(hΦ : IsStreamSeq I Φ)
(m : ℕ)
(κm : ℝ)
{k : ℤ}
(hk : Odd k)
:
Continuous (leadingSummand I hΦ m κm k)
theorem
AVenhance.Infra.Section5.LeftToShow.leadingMatrix_continuous
{β : ℝ}
(I : Ingredients β)
{Φ : ℕ → ℝ → Homogenization.Vec 2 → ℝ}
(hΦ : IsStreamSeq I Φ)
{m : ℕ}
(_hm : 1 ≤ m)
{κm : ℝ}
(_hκm : 0 < κm)
:
Continuous fun (p : ℝ × Homogenization.Vec 2) => leadingMatrix I hΦ m κm p.1 p.2
Joint continuity of F (finitely many active modes near each time).