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Exponential C0C^0C0 convergence of asymptotically cylindrical ends at nondegenerate orbits

Proved
FiniteEnergyPlane.exists_expDecay_of_isAsymptoticallyCylindricalEnd

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, 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}, P=(x,T)P=(x,T)P=(x,T) a nondegenerate periodic Reeb orbit and ε=±1\varepsilon=\pm1ε=±1. 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 projection of uuu. Suppose that for some constants d,cd,cd,c both a(s,t)−εTs−da(s,t)-\varepsilon Ts-da(s,t)−εTs−d and w(s,t)−x(εTt+c)w(s,t)-x(\varepsilon Tt+c)w(s,t)−x(εTt+c) tend to 000 in C∞C^\inftyC∞, uniformly in ttt, as s→+∞s\to+\inftys→+∞. Then there are δ>0\delta>0δ>0, CCC and s0s_0s0​ such that for all s≥s0s\ge s_0s≥s0​ and all ttt,

∣a(s,t)−εTs−d∣≤Ce−δs,∥w(s,t)−x(εTt+c)∥≤Ce−δs.|a(s,t)-\varepsilon Ts-d|\le Ce^{-\delta s},\qquad \|w(s,t)-x(\varepsilon Tt+c)\|\le Ce^{-\delta s}.∣a(s,t)−εTs−d∣≤Ce−δs,∥w(s,t)−x(εTt+c)∥≤Ce−δs.

This is the C0C^0C0 part of the exponential convergence of nondegenerate ends (Hryniewicz, Theorem 2.10), with the same constants d,cd,cd,c as in the hypothesis.

Formalization Note The hypotheses are the two TendstoZeroCInfty conditions of IsAsymptoticallyCylindricalEnd H u cylEnd P ε with the constants d,cd,cd,c made explicit; aaa and www are endA H u cylEnd and endW H u cylEnd, and the norm on VVV is the sup norm.

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}` that is asymptotically
cylindrical over a nondegenerate periodic Reeb orbit `P` with sign `ε`, with constants `d, c`, in
the cylindrical coordinates `cylEnd` at the puncture. Then both `a(s, t) - εTs - d` and
`w(s, t) - x(εTt + c)` decay like `e^{-δs}` uniformly in `t`, for some `δ > 0`. -/
theorem exists_expDecay_of_isAsymptoticallyCylindricalEnd {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) (hP : P.IsNondegenerate)
    (ε : ℝ) (hε : ε = 1 ∨ ε = -1) (d c : ℝ)
    (ha : TendstoZeroCInfty (fun p : ℝ × ℝ => endA H u cylEnd p - ε * P.T * p.1 - d))
    (hw : TendstoZeroCInfty (fun p : ℝ × ℝ => endW H u cylEnd p - P.x (ε * P.T * p.2 + c))) :
    ∃ δ > 0, ∃ C s₀ : ℝ, ∀ s ≥ s₀, ∀ t : ℝ,
      |endA H u cylEnd (s, t) - ε * P.T * s - d| ≤ C * Real.exp (-(δ * s)) ∧
        ‖endW H u cylEnd (s, t) - P.x (ε * P.T * t + c)‖ ≤ C * Real.exp (-(δ * s)) := by
  sorry

end FiniteEnergyPlane
Source
U. Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, 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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