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An end with nonvanishing dλ-density is not a reparametrized Reeb orbit

Proved
FiniteEnergyPlane.exists_endW_ne_proj_reeb_comp

by Mazecto · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

asymptotic-analysispseudoholomorphic-curvesreeb-dynamicssymplectization

Let uuu be a finite-energy J~\tilde JJ~-holomorphic curve on D∖{0}D\setminus\{0\}D∖{0} (strictly star-shaped level S=H−1(1)S=H^{-1}(1)S=H−1(1), compatible JJJ), and suppose that the density ω0(∂sw,∂tw)\omega_0(\partial_sw,\partial_tw)ω0​(∂s​w,∂t​w), w=proj∘uw=\mathrm{proj}\circ uw=proj∘u, does not vanish identically on any punctured disk Br(0)∖{0}B_r(0)\setminus\{0\}Br​(0)∖{0}. Let P=(x,T)P=(x,T)P=(x,T) be a periodic Reeb orbit and τ:R2→R\tau:\mathbb{R}^2\to\mathbb{R}τ:R2→R of class C1C^1C1 on some (sτ,∞)×R(s_\tau,\infty)\times\mathbb{R}(sτ​,∞)×R. Then for every s0s_0s0​ there are s≥s0s\ge s_0s≥s0​ and ttt with

w(e−2π(s+it))≠proj x(τ(s,t)).w\big(e^{-2\pi(s+it)}\big)\ne\mathrm{proj}\,x(\tau(s,t)).w(e−2π(s+it))=projx(τ(s,t)).

So such a curve is not, on any end, a reparametrization of the trivial cylinder over PPP.

Formalization Note The density is dlambdaDensity H u z; the end is endW H u cylEnd (s, t).

Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- A finite-energy curve on `D \ {0}` whose `dλ`-density `ω₀(∂ₛw, ∂ₜw)` (`w = proj H ∘ u`) does
not vanish identically on any punctured neighbourhood of `0` is not, on any end `s ≥ s₀`, of the
form `w(s, t) = proj H (x(τ(s, t)))` with `x` a Reeb orbit and `τ` of class `C¹`: for every `s₀`
there are `s ≥ s₀` and `t` with `endW(s, t) ≠ proj H (x(τ(s, t)))`. -/
theorem exists_endW_ne_proj_reeb_comp {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)
    (hden : ∀ r > 0, ∃ z ∈ ball (0 : ℂ) r \ {0}, dlambdaDensity H u z ≠ 0)
    (τ : ℝ × ℝ → ℝ) (sτ : ℝ) (hτ : ContDiffOn ℝ 1 τ (Set.Ioi sτ ×ˢ Set.univ)) :
    ∀ s₀ : ℝ, ∃ s ≥ s₀, ∃ t : ℝ, endW H u cylEnd (s, t) ≠ proj H (P.x (τ (s, t))) := by
  sorry

end FiniteEnergyPlane
Source
Used for 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 2.11 and Lemma 2.12; H. Hofer, K. Wysocki, E. Zehnder, Properties of pseudoholomorphic curves in symplectisations I: asymptotics, Ann. Inst. H. Poincaré Anal. Non Linéaire 13 (1996)

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