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Ends at nondegenerate orbits converge with a fixed phase

Proved
FiniteEnergyPlane.exists_tendsto_cylEnd_of_isNondegenerate

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 σ=±1\sigma=\pm1σ=±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 of uuu and w(s,t)∈Sw(s,t)\in Sw(s,t)∈S for its projection. Assume:

  1. for every m≥1m\ge1m≥1, the mmm-th derivative of (s,t)↦a(s,t)−σTs(s,t)\mapsto a(s,t)-\sigma Ts(s,t)↦a(s,t)−σTs tends to 000 as s→+∞s\to+\inftys→+∞, uniformly in ttt;
  2. for every m≥0m\ge0m≥0 and ε>0\varepsilon>0ε>0 there is s1s_1s1​ such that for every s≥s1s\ge s_1s≥s1​ some c′∈Rc'\in\mathbb{R}c′∈R satisfies ∥Dj(w−x(σT ⋅2+c′))(s,t)∥≤ε\|D^j\big(w-x(\sigma T\,\cdot_2+c')\big)(s,t)\|\le\varepsilon∥Dj(w−x(σT⋅2​+c′))(s,t)∥≤ε for all ttt and all j≤mj\le mj≤m.

Then there are constants d,c∈Rd,c\in\mathbb{R}d,c∈R such that, uniformly in ttt as s→+∞s\to+\inftys→+∞,

a(s,t)−σTs−d→0,w(s,t)−x(σTt+c)→0.a(s,t)-\sigma Ts-d\to0,\qquad w(s,t)-x(\sigma Tt+c)\to0.a(s,t)−σTs−d→0,w(s,t)−x(σTt+c)→0.

So at a nondegenerate orbit, convergence of the end to the trivial cylinder up to an sss-dependent phase and an additive constant improves to convergence with one fixed phase ccc and one fixed constant ddd.

Formalization Note aaa and www are endA H u cylEnd and endW H u cylEnd; derivatives are iteratedFDeriv ℝ on R×R\mathbb{R}\times\mathbb{R}R×R with the sup norm on R2n+2\mathbb{R}^{2n+2}R2n+2; uniform convergence is TendstoZeroUnif. In hypothesis 2, x(σT ⋅2+c′)x(\sigma T\,\cdot_2+c')x(σT⋅2​+c′) is the map (s,t)↦x(σTt+c′)(s,t)\mapsto x(\sigma Tt+c')(s,t)↦x(σTt+c′).

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}`, `P = (x, T)` a nondegenerate
periodic Reeb orbit and `σ = ±1`. In the cylindrical coordinates `cylEnd` at `0`, suppose every
derivative of order `≥ 1` of `a(s, t) - σ T s` tends to `0` uniformly in `t`, and that for every
`m` and `ε > 0`, for all large `s` there is a phase `c'` such that the derivatives of order `≤ m`
of `w - x(σ T t + c')` at `(s, t)` are at most `ε` for all `t`. Then there are constants `d, c`
with `a(s, t) - σ T s - d → 0` and `w(s, t) - x(σ T t + c) → 0` uniformly in `t`. -/
theorem exists_tendsto_cylEnd_of_isNondegenerate {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)
    (σ : ℝ) (hσ : σ = 1 ∨ σ = -1)
    (hA : ∀ m : ℕ, 1 ≤ m → ∀ ε > 0, ∃ s₁ : ℝ, ∀ s ≥ s₁, ∀ t : ℝ,
      ‖iteratedFDeriv ℝ m (fun p : ℝ × ℝ => endA H u cylEnd p - σ * P.T * p.1) (s, t)‖ ≤ ε)
    (hW : ∀ m : ℕ, ∀ ε > 0, ∃ s₁ : ℝ, ∀ s ≥ s₁, ∃ c' : ℝ, ∀ j ≤ m, ∀ t : ℝ,
      ‖iteratedFDeriv ℝ j
        (fun p : ℝ × ℝ => endW H u cylEnd p - P.x (σ * P.T * p.2 + c')) (s, t)‖ ≤ ε) :
    ∃ d c : ℝ,
      TendstoZeroUnif (fun p : ℝ × ℝ => endA H u cylEnd p - σ * P.T * p.1 - d) ∧
        TendstoZeroUnif (fun p : ℝ × ℝ => endW H u cylEnd p - P.x (σ * P.T * p.2 + c)) := by
  sorry

end FiniteEnergyPlane
Source
H. Hofer, K. Wysocki, E. Zehnder, Properties of pseudoholomorphic curves in symplectisations I: Asymptotics, Ann. Inst. H. Poincaré Anal. Non Linéaire 13 (1996), 337–379, with the Correction, ibid. 15 (1998), 535–538, Lemmas 2.6 and 2.7

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