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A finite-energy curve with one positive prime puncture, negative punctures and no dλd\lambdadλ-energy is a trivial cylinder

Proved
FiniteEnergyPlane.exists_eq_singleton_of_dlambdaEnergy_eq_zero

by Mazecto · Nov 4, 2026 · Mathlib 0df444a (Lean v4.33.1)

pseudoholomorphic-curvesreeb-dynamicssymplectization

Let www be a finite-energy J~\tilde JJ~-holomorphic curve on C∖Γ\mathbb{C}\setminus\GammaC∖Γ, Γ\GammaΓ finite, in the symplectization of a strictly star-shaped level S⊂R4S\subset\mathbb{R}^4S⊂R4. Suppose www has a nondegenerate positive puncture at ∞\infty∞ over a prime periodic Reeb orbit P=(x,T)P=(x,T)P=(x,T), the action of www on circles of radius ρ\rhoρ tends to TTT as ρ→∞\rho\to\inftyρ→∞, the coordinate a∘wa\circ wa∘w tends to −∞-\infty−∞ at every point of Γ\GammaΓ, and ∫C∖Γw∗dλ=0\int_{\mathbb{C}\setminus\Gamma}w^*d\lambda=0∫C∖Γ​w∗dλ=0. Then Γ\GammaΓ is a single point z1z_1z1​; for every z≠z1z\ne z_1z=z1​ the projection of w(z)w(z)w(z) to SSS lies on the image of xxx and π ∂spr(w)(z)=0\pi\,\partial_s\mathrm{pr}(w)(z)=0π∂s​pr(w)(z)=0; and the action of www on every circle ∣z∣=ρ>∣z1∣|z|=\rho>|z_1|∣z∣=ρ>∣z1​∣ equals TTT.

This identifies the dλd\lambdadλ-energy-free limits that occur in the compactness theory of fast planes.

Formalization Note IsNondegenerateEnd H w cylInf P 1, P.IsPrime, piDs H w z and loopAction H w (ccwLoop ρ) are the published objects; the dλd\lambdadλ-energy is dlambdaEnergy H (↑Γ)ᶜ w.

Preamble
import Definitions.Def_FiniteEnergyPlane_Compactness
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Let `w` be a finite-energy `J̃`-holomorphic curve on `ℂ \ Γ`, `Γ` finite, in the symplectization of
`S ⊂ ℝ⁴`, with vanishing `dλ`-energy, `aCoord H ∘ w → -∞` at every point of `Γ`, and a nondegenerate
positive puncture at `∞` over a prime orbit `P` with `∫_{|z| = ρ} w*λ → P.T` as `ρ → ∞`. Then `Γ` is a
single point `z₁`, the projection of `w` lies in the image of `P`, `π ∂ₛw` vanishes identically, and
`∫_{|z| = ρ} w*λ = P.T` for every `ρ > ‖z₁‖`. -/
theorem exists_eq_singleton_of_dlambdaEnergy_eq_zero (H : V 1 → ℝ)
    (hH : IsStrictlyStarShapedLevel H) (J : V 1 → V 1 →L[ℝ] V 1) (hJ : IsCompatibleXiStructure H J)
    (Γ : Finset ℂ) (w : ℂ → V 1) (hw : IsFiniteEnergyCurve H J (↑Γ)ᶜ w)
    (P : ReebOrbit H) (hprime : P.IsPrime) (hinf : IsNondegenerateEnd H w cylInf P 1)
    (hact : Tendsto (fun ρ : ℝ => loopAction H w (ccwLoop ρ)) atTop (𝓝 P.T))
    (hneg : ∀ z₀ ∈ Γ, Tendsto (fun z => aCoord H (w z)) (𝓝[≠] z₀) atBot)
    (hzero : dlambdaEnergy H (↑Γ)ᶜ w = 0) :
    ∃ z₁ : ℂ, Γ = {z₁} ∧ (∀ z ∉ Γ, proj H (w z) ∈ Set.range P.x ∧ piDs H w z = 0) ∧
      ∀ ρ : ℝ, ‖z₁‖ < ρ → loopAction H w (ccwLoop ρ) = P.T := by
  sorry

end FiniteEnergyPlane
Source
U. Hryniewicz, Trans. AMS 364 (2012), arXiv:0812.4076, Section 4 (Lemma 4.17 and its proof)

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