Tangential Cauchy–Riemann defect of an end in tube coordinates
ProvedFiniteEnergyPlane.exists_dbar_bound_tubeTangentLet be a strictly star-shaped level with contact planes , a smooth -compatible complex structure on , a finite-energy -holomorphic curve on and a periodic Reeb orbit, , . In the cylindrical coordinates at write for the symplectization coordinate and for the radial projection of . Suppose that for
with and , where and in , uniformly in , as . Let and put and . Then there are and such that for all and all
That is, is holomorphic in up to an error controlled by and its first derivative. This describes the directions of an end tangent to the trivial cylinder (Hryniewicz, Theorem 2.10; Wendl, Proposition 6.7.1).
Formalization Note proj H is the radial projection onto , IsInXi H x v means , and convergence is TendstoZeroCInfty (smooth on some , every derivative tends to uniformly in ). and are endA H u cylEnd and endW H u cylEnd; norms on are sup norms. Partial derivatives are fderiv ℝ _ (s, t) (1, 0) and fderiv ℝ _ (s, t) (0, 1), and is the operator norm of fderiv ℝ h (s, t).
import Definitions.Def_FiniteEnergyPlane_Asymptotics
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real
/-- Let `u` be a finite-energy `J̃`-holomorphic curve on `D \ {0}` and `P = (x, T)` a periodic Reeb
orbit. Suppose that, in the cylindrical coordinates `cylEnd` at `0` and for `s ≥ s₀`,
`w = proj H (x(τ) + h)` with `h ∈ ξ_{x(τ)}`, `τ(s, t + 1) = τ(s, t) + εT` and `h` `1`-periodic,
where `τ(s, t) - εTt - c → 0` and `h → 0` in `C^∞`. Put `f = a - εTs - d` and `g = τ - εTt - c`.
Then `f + i g` is holomorphic in `s + it` up to an error controlled by `h`:
`|∂ₛf - ∂ₜg| + |∂ₜf + ∂ₛg| ≤ K (‖h‖ + ‖Dh‖)` for `s ≥ s₁`. -/
theorem exists_dbar_bound_tubeTangent {n : ℕ} (H : V n → ℝ) (hH : IsStrictlyStarShapedLevel H)
(J : V n → V n →L[ℝ] V n) (hJ : IsCompatibleXiStructure H J) (u : ℂ → V n)
(hu : IsFiniteEnergyCurve H J (ball 0 1 \ {0}) u) (P : ReebOrbit H)
(ε : ℝ) (hε : ε = 1 ∨ ε = -1) (d c : ℝ) (τ : ℝ × ℝ → ℝ) (h : ℝ × ℝ → V n) (s₀ : ℝ)
(hτ : TendstoZeroCInfty (fun p : ℝ × ℝ => τ p - ε * P.T * p.2 - c))
(hh : TendstoZeroCInfty h)
(hrep : ∀ s ≥ s₀, ∀ t : ℝ,
τ (s, t + 1) = τ (s, t) + ε * P.T ∧ h (s, t + 1) = h (s, t) ∧
IsInXi H (P.x (τ (s, t))) (h (s, t)) ∧
endW H u cylEnd (s, t) = proj H (P.x (τ (s, t)) + h (s, t))) :
∃ K s₁ : ℝ, ∀ s ≥ s₁, ∀ t : ℝ,
|fderiv ℝ (fun p : ℝ × ℝ => endA H u cylEnd p - ε * P.T * p.1 - d) (s, t) (1, 0) -
fderiv ℝ (fun p : ℝ × ℝ => τ p - ε * P.T * p.2 - c) (s, t) (0, 1)| +
|fderiv ℝ (fun p : ℝ × ℝ => endA H u cylEnd p - ε * P.T * p.1 - d) (s, t) (0, 1) +
fderiv ℝ (fun p : ℝ × ℝ => τ p - ε * P.T * p.2 - c) (s, t) (1, 0)| ≤
K * (‖h (s, t)‖ + ‖fderiv ℝ h (s, t)‖) := by
sorry
end FiniteEnergyPlane