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LeanPool.AnomalousDiffusion.AVenhance.Infra.Section5.RelativeError.ForcedEnergyDrift

Divergence-free transport cancellation along a path #

For a bounded measurable divergence-free periodic drift and a path that is periodic H¹ for almost every time, the transport pairing ∫ b·Dw w vanishes on every truncated time cell. This is the statement of weak_solution_divFree_drift_pairing_zero without the weak-equation hypothesis.

The transport density of a bounded drift against an L² gradient is in L².

theorem AVenhance.Infra.Section5.RelativeError.drift_pairing_region_zero {b : ℝ → Homogenization.Vec 2 → Homogenization.Vec 2} {w : ℝ → Homogenization.Vec 2 → ℝ} {Dw : ℝ → Homogenization.Vec 2 → Homogenization.Vec 2} (hw : MeasureTheory.MemLp (fun (p : ℝ × Homogenization.Vec 2) => w p.1 p.2) 2 (MeasureTheory.volume.restrict timeCube)) (hDw : ∀ (i : Fin 2), MeasureTheory.MemLp (fun (p : ℝ × Homogenization.Vec 2) => Dw p.1 p.2 i) 2 (MeasureTheory.volume.restrict timeCube)) (hH1 : ∀ᵐ (s : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo 0 1), IsPeriodicH1With (w s) (Dw s)) (hb_meas : MeasureTheory.AEStronglyMeasurable (fun (p : ℝ × Homogenization.Vec 2) => b p.1 p.2) (MeasureTheory.volume.restrict (Set.Icc 0 1 ×ˢ Set.univ))) (hb_bdd : ∃ (C : ℝ), ∀ t ∈ Set.Icc 0 1, ∀ (x : Homogenization.Vec 2), ‖b t x‖ ≤ C) (hb_per : ∀ t ∈ Set.Icc 0 1, IsZ2Periodic (b t)) (hdiv : IsDivFree b) {t : ℝ} (ht : t ∈ Set.Icc 0 1) :

Divergence-free transport cancels on every truncated time cell for an H¹ path.