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Tangential Cauchy–Riemann defect of an end in tube coordinates

Proved
FiniteEnergyPlane.exists_dbar_bound_tubeTangent

by Mazecto · Oct 29, 2026 · Mathlib 0df444a (Lean v4.33.1)

asymptotic-analysispseudoholomorphic-curvesreeb-dynamicssymplectization

Let S=H−1(1)⊂R2n+2S=H^{-1}(1)\subset\mathbb{R}^{2n+2}S=H−1(1)⊂R2n+2 be a strictly star-shaped level with contact planes ξ\xiξ, JJJ a smooth dλ0d\lambda_0dλ0​-compatible complex structure on ξ\xiξ, uuu a finite-energy J~\tilde JJ~-holomorphic curve on D∖{0}D\setminus\{0\}D∖{0} and P=(x,T)P=(x,T)P=(x,T) a periodic Reeb orbit, ε=±1\varepsilon=\pm1ε=±1, c∈Rc\in\mathbb{R}c∈R. In the cylindrical coordinates e−2π(s+it)e^{-2\pi(s+it)}e−2π(s+it) at 000 write a(s,t)a(s,t)a(s,t) for the symplectization coordinate and w(s,t)∈Sw(s,t)\in Sw(s,t)∈S for the radial projection of uuu. Suppose that for s≥s0s\ge s_0s≥s0​

w(s,t)=proj(x(τ(s,t))+h(s,t)),h(s,t)∈ξx(τ(s,t)),w(s,t)=\mathrm{proj}\big(x(\tau(s,t))+h(s,t)\big),\qquad h(s,t)\in\xi_{x(\tau(s,t))},w(s,t)=proj(x(τ(s,t))+h(s,t)),h(s,t)∈ξx(τ(s,t))​,

with τ(s,t+1)=τ(s,t)+εT\tau(s,t+1)=\tau(s,t)+\varepsilon Tτ(s,t+1)=τ(s,t)+εT and h(s,t+1)=h(s,t)h(s,t+1)=h(s,t)h(s,t+1)=h(s,t), where τ(s,t)−εTt−c→0\tau(s,t)-\varepsilon Tt-c\to0τ(s,t)−εTt−c→0 and h→0h\to0h→0 in C∞C^\inftyC∞, uniformly in ttt, as s→+∞s\to+\inftys→+∞. Let d∈Rd\in\mathbb{R}d∈R and put f=a−εTs−df=a-\varepsilon Ts-df=a−εTs−d and g=τ−εTt−cg=\tau-\varepsilon Tt-cg=τ−εTt−c. Then there are KKK and s1s_1s1​ such that for all s≥s1s\ge s_1s≥s1​ and all ttt

∣∂sf−∂tg∣+∣∂tf+∂sg∣≤K(∥h∥+∥Dh∥)(s,t).|\partial_sf-\partial_tg|+|\partial_tf+\partial_sg|\le K\big(\|h\|+\|Dh\|\big)(s,t).∣∂s​f−∂t​g∣+∣∂t​f+∂s​g∣≤K(∥h∥+∥Dh∥)(s,t).

That is, f+igf+igf+ig is holomorphic in s+its+its+it up to an error controlled by hhh 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 SSS, IsInXi H x v means v∈ξx=ker⁡λ0(x)∩ker⁡dH(x)v\in\xi_x=\ker\lambda_0(x)\cap\ker dH(x)v∈ξx​=kerλ0​(x)∩kerdH(x), and C∞C^\inftyC∞ convergence is TendstoZeroCInfty (smooth on some (s0,∞)×R(s_0,\infty)\times\mathbb{R}(s0​,∞)×R, every derivative tends to 000 uniformly in ttt). aaa and www are endA H u cylEnd and endW H u cylEnd; norms on V=R2n+2V=\mathbb{R}^{2n+2}V=R2n+2 are sup norms. Partial derivatives are fderiv ℝ _ (s, t) (1, 0) and fderiv ℝ _ (s, t) (0, 1), and ∥Dh∥\|Dh\|∥Dh∥ is the operator norm of fderiv ℝ h (s, t).

Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
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
Source
U. Hryniewicz, J. Symplectic Geom. 12 (2014), arXiv:1105.2077, Theorem 2.10; H. Hofer, K. Wysocki, E. Zehnder, Properties of pseudoholomorphic curves in symplectisations I: asymptotics, Ann. Inst. H. Poincaré Anal. Non Linéaire 13 (1996); C. Wendl, Lectures on Symplectic Field Theory (2026 notes), Proposition 6.7.1

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