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Fixed-phase C0C^0C0 convergence and C∞C^\inftyC∞ convergence up to phase give C∞C^\inftyC∞ convergence

Proved
FiniteEnergyPlane.tendstoZeroCInfty_of_tendstoZeroUnif_mod_phase

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

asymptotic-analysisreal-analysisreeb-dynamics

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, P=(x,T)P=(x,T)P=(x,T) a periodic Reeb orbit on SSS and σ=±1\sigma=\pm1σ=±1. Let A:R2→RA:\mathbb{R}^2\to\mathbb{R}A:R2→R and W:R2→R2n+2W:\mathbb{R}^2\to\mathbb{R}^{2n+2}W:R2→R2n+2 be C∞C^\inftyC∞ on (s0,∞)×R(s_0,\infty)\times\mathbb{R}(s0​,∞)×R for some s0s_0s0​, and d,c∈Rd,c\in\mathbb{R}d,c∈R. 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;
  3. A(s,t)−σTs−d→0A(s,t)-\sigma Ts-d\to0A(s,t)−σTs−d→0 and W(s,t)−x(σTt+c)→0W(s,t)-x(\sigma Tt+c)\to0W(s,t)−x(σTt+c)→0 as s→+∞s\to+\inftys→+∞, uniformly in ttt.

Then (s,t)↦A(s,t)−σTs−d(s,t)\mapsto A(s,t)-\sigma Ts-d(s,t)↦A(s,t)−σTs−d and (s,t)↦W(s,t)−x(σTt+c)(s,t)\mapsto W(s,t)-x(\sigma Tt+c)(s,t)↦W(s,t)−x(σTt+c) tend to 000 in C∞C^\inftyC∞: both are smooth on some (s0′,∞)×R(s_0',\infty)\times\mathbb{R}(s0′​,∞)×R, and every derivative of each tends to 000 uniformly in ttt.

This combines convergence up to a phase in all derivatives with uniform convergence at a fixed phase into C∞C^\inftyC∞ convergence at that fixed phase, which is the form of the conclusion of asymptotic cylindricity.

Formalization Note 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; the conclusion is TendstoZeroCInfty for both maps. 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′). PPP may be multiply covered.

Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Let `P = (x, T)` be a periodic Reeb orbit, `σ = ±1`, and `A : ℝ × ℝ → ℝ`, `W : ℝ × ℝ → V n`
smooth on some `(s₀, ∞) × ℝ`. Suppose every derivative of order `≥ 1` of `A(s, t) - σ T s` tends to
`0` uniformly in `t`; 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`; and
`A(s, t) - σ T s - d → 0`, `W(s, t) - x(σ T t + c) → 0` uniformly in `t`. Then both
`A(s, t) - σ T s - d` and `W(s, t) - x(σ T t + c)` tend to `0` in `C^∞`. -/
theorem tendstoZeroCInfty_of_tendstoZeroUnif_mod_phase {n : ℕ} (H : V n → ℝ)
    (hH : IsStrictlyStarShapedLevel H) (P : ReebOrbit H) (σ : ℝ) (hσ : σ = 1 ∨ σ = -1)
    (A : ℝ × ℝ → ℝ) (W : ℝ × ℝ → V n)
    (hsm : ∃ s₀ : ℝ, ContDiffOn ℝ ∞ A (Set.Ioi s₀ ×ˢ Set.univ) ∧
      ContDiffOn ℝ ∞ W (Set.Ioi s₀ ×ˢ Set.univ))
    (hA : ∀ m : ℕ, 1 ≤ m → ∀ ε > 0, ∃ s₁ : ℝ, ∀ s ≥ s₁, ∀ t : ℝ,
      ‖iteratedFDeriv ℝ m (fun p : ℝ × ℝ => A 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 => W p - P.x (σ * P.T * p.2 + c')) (s, t)‖ ≤ ε)
    (d c : ℝ) (hA0 : TendstoZeroUnif (fun p : ℝ × ℝ => A p - σ * P.T * p.1 - d))
    (hW0 : TendstoZeroUnif (fun p : ℝ × ℝ => W p - P.x (σ * P.T * p.2 + c))) :
    TendstoZeroCInfty (fun p : ℝ × ℝ => A p - σ * P.T * p.1 - d) ∧
      TendstoZeroCInfty (fun p : ℝ × ℝ => W 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, proof of Theorem 1.3

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