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Shifted cylindrical coordinates of an end converge in Cloc∞C^\infty_{loc}Cloc∞​ to a trivial cylinder

Proved
FiniteEnergyPlane.exists_subseq_tendstoCInftyLocOn_cylEnd_shift

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 form λ=λ0∣S\lambda=\lambda_0|_Sλ=λ0​∣S​, Reeb field RRR and a dλd\lambdadλ-compatible complex structure JJJ on ξ\xiξ, and let u=(a,w):D˙=D∖{0}→R×S≅R2n+2∖{0}u=(a,w):\dot D=D\setminus\{0\}\to\mathbb{R}\times S\cong\mathbb{R}^{2n+2}\setminus\{0\}u=(a,w):D˙=D∖{0}→R×S≅R2n+2∖{0} be a finite-energy J~\tilde JJ~-holomorphic curve on the punctured unit disc. Let P=(x,T)P=(x,T)P=(x,T) be a periodic Reeb orbit (degenerate orbits allowed) and σ∈{1,−1}\sigma\in\{1,-1\}σ∈{1,−1}. Write a(s,t)a(s,t)a(s,t), w(s,t)w(s,t)w(s,t) for the components of u(e−2π(s+it))u(e^{-2\pi(s+it)})u(e−2π(s+it)) in the cylindrical coordinates at the puncture.

Assume that for every ε>0\varepsilon>0ε>0 there is r0>0r_0>0r0​>0 such that for each 0<r<r00<r<r_00<r<r0​ some phase c′c'c′ satisfies

sup⁡t∥w(re−2πit)−x(σTt+c′)∥≤ε.\sup_{t}\big\|w\big(r e^{-2\pi i t}\big)-x(\sigma T t+c')\big\|\le\varepsilon .tsup​​w(re−2πit)−x(σTt+c′)​≤ε.

Then for every sequence sj→∞s_j\to\inftysj​→∞ there are a subsequence (not relabelled) and a phase c∈Rc\in\mathbb{R}c∈R such that

a(s+sj,t)−a(sj,0)⟶σTs,w(s+sj,t)⟶x(σTt+c)a(s+s_j,t)-a(s_j,0)\longrightarrow \sigma T s,\qquad w(s+s_j,t)\longrightarrow x(\sigma T t+c)a(s+sj​,t)−a(sj​,0)⟶σTs,w(s+sj​,t)⟶x(σTt+c)

in Cloc∞(R2)C^\infty_{loc}(\mathbb{R}^2)Cloc∞​(R2), i.e. with all derivatives, uniformly on compact subsets of R2\mathbb{R}^2R2.

This is the compactness statement behind the C∞C^\inftyC∞ convergence, up to phase, of the end (a,w)(a,w)(a,w) to the trivial cylinder over PPP.

Formalization Note endA H u cylEnd and endW H u cylEnd are aaa and www in the coordinates cylEnd s t =e−2π(s+it)=e^{-2\pi(s+it)}=e−2π(s+it); the shifted maps are p ↦ endA H u cylEnd (p + (s_j, 0)) - endA H u cylEnd (s_j, 0) and p ↦ endW H u cylEnd (p + (s_j, 0)) on ℝ × ℝ. Cloc∞C^\infty_{loc}Cloc∞​ convergence is JHolomorphic.TendstoCInftyLocOn on Set.univ; the subsequence is a strictly monotone φ. The loop hypothesis uses loopInS H u (cwLoop 0 r), eventually in 𝓝[>] 0.

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 periodic Reeb
orbit and `σ = ±1`. Suppose that for every `ε > 0`, every clockwise loop
`t ↦ proj(u(r e^{-2π i t}))` of sufficiently small radius `r > 0` is uniformly `ε`-close to some
reparametrization `t ↦ x(σ T t + c')`. Then for every sequence `s_j → ∞` there are a subsequence
and a phase `c` such that, in the cylindrical coordinates `cylEnd` at `0`, the shifted maps
`(s, t) ↦ a(s + s_j, t) - a(s_j, 0)` converge in `C^∞_loc(ℝ²)` to `(s, t) ↦ σ T s`, and the shifted
maps `(s, t) ↦ w(s + s_j, t)` converge in `C^∞_loc(ℝ²)` to `(s, t) ↦ x(σ T t + c)`. -/
theorem exists_subseq_tendstoCInftyLocOn_cylEnd_shift {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) (σ : ℝ)
    (hσ : σ = 1 ∨ σ = -1)
    (hloop : ∀ ε : ℝ, 0 < ε → ∀ᶠ r in 𝓝[>] (0 : ℝ), ∃ c' : ℝ, ∀ t : ℝ,
      ‖loopInS H u (cwLoop 0 r) t - P.x (σ * P.T * t + c')‖ ≤ ε)
    (s : ℕ → ℝ) (hs : Tendsto s atTop atTop) :
    ∃ φ : ℕ → ℕ, StrictMono φ ∧ ∃ c : ℝ,
      JHolomorphic.TendstoCInftyLocOn
        (fun j (p : ℝ × ℝ) => endA H u cylEnd (p + (s (φ j), 0)) - endA H u cylEnd (s (φ j), 0))
        (fun p => σ * P.T * p.1) Set.univ ∧
      JHolomorphic.TendstoCInftyLocOn
        (fun j (p : ℝ × ℝ) => endW H u cylEnd (p + (s (φ j), 0)))
        (fun p => P.x (σ * P.T * p.2 + c)) Set.univ := 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, Lemma 2.4 and its proof

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