All-order forcing-gradient energy from preceding L2 gradient energies.
theorem
AVenhance.Infra.Section4.iterate_word_forcing_energy_bound
{A : ℝ → Homogenization.Vec 2 → Matrix (Fin 2) (Fin 2) ℝ}
{v : ℝ → Homogenization.Vec 2 → ℝ}
(hv : ContDiffOn ℝ (↑⊤) (fun (z : AmnrSpace) => v z.1 z.2) (Set.Ici 0 ×ˢ Set.univ))
(hA : ∀ (t : ℝ), 0 < t → ContDiff ℝ (↑⊤) (A t))
(hcoef :
∀ (r : List (Fin 2)), ContinuousOn (fun (z : AmnrSpace) => iterateMatrixWord (A z.1) r z.2) (Set.Ici 0 ×ˢ Set.univ))
(w : List (Fin 2))
(D E : ℕ → ℝ)
(hD :
∀ (t : ℝ) (x : Homogenization.Vec 2) (r : List (Fin 2)) (j k : Fin 2), |iterateMatrixWord (A t) r x j k| ≤ D r.length)
(hE :
∀ (r : List (Fin 2)),
r.length ≤ w.length + 2 → (spaceTimeGradNormSq fun (t : ℝ) => spaceGrad (iterateSpatialWord r (v t))) ≤ E r.length)
(hFI :
MeasureTheory.IntegrableOn
(fun (z : AmnrSpace) =>
Homogenization.vecNormSq
(spaceGrad
(iterateSpatialWord w (vecDiv fun (y : Homogenization.Vec 2) => (A z.1 y).mulVec (spaceGrad (v z.1) y))) z.2))
timeCube MeasureTheory.volume)
:
Integrate the explicit forcing-gradient expansion. The only quantitative scalar premise concerns the preceding field's actual gradient energies.