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The asymptotic-operator expression of a contact-plane section stays in the contact plane

Proved
FiniteEnergyPlane.isInXi_linearizedReeb_deriv

by Mazecto · Oct 30, 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 planes ξ\xiξ, P=(x,T)P=(x,T)P=(x,T) a periodic Reeb orbit, and η:R→R2n+2\eta:\mathbb{R}\to\mathbb{R}^{2n+2}η:R→R2n+2 differentiable with η(t)∈ξx(Tt)\eta(t)\in\xi_{x(Tt)}η(t)∈ξx(Tt)​ for all ttt. Then for all ttt,

−η′(t)+T DR(x(Tt)) η(t)∈ξx(Tt).-\eta'(t)+T\,DR(x(Tt))\,\eta(t)\in\xi_{x(Tt)}.−η′(t)+TDR(x(Tt))η(t)∈ξx(Tt)​.

This is the expression to which JJJ is applied in the asymptotic operator APη=J(−η′+T DR η)A_P\eta=J(-\eta'+T\,DR\,\eta)AP​η=J(−η′+TDRη), so the statement says that APA_PAP​ is well defined on sections of ξ\xiξ along PPP.

Formalization Note V n is R2n+2\mathbb{R}^{2n+2}R2n+2, IsStrictlyStarShapedLevel H says HHH is smooth and S=H−1(1)S=H^{-1}(1)S=H−1(1) is strictly star-shaped with dH(x)x>0dH(x)x>0dH(x)x>0 on SSS, reeb H is the Reeb field R=XH/λ0(XH)R=X_H/\lambda_0(X_H)R=XH​/λ0​(XH​), liouville x v is λ0(x)v=12ω0(x,v)\lambda_0(x)v=\tfrac12\omega_0(x,v)λ0​(x)v=21​ω0​(x,v), IsInXi H x v means v∈ξx=ker⁡λ0(x)∩ker⁡dH(x)v\in\xi_x=\ker\lambda_0(x)\cap\ker dH(x)v∈ξx​=kerλ0​(x)∩kerdH(x), and a ReebOrbit H is P=(x,T)P=(x,T)P=(x,T) with x′=R(x)x'=R(x)x′=R(x), x(R)⊂Sx(\mathbb{R})\subset Sx(R)⊂S, x(τ+T)=x(τ)x(\tau+T)=x(\tau)x(τ+T)=x(τ), T>0T>0T>0.

Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
namespace FiniteEnergyPlane

/-- Let `P = (x, T)` be a periodic Reeb orbit and `η` a differentiable family with
`η(t) ∈ ξ_{x(Tt)}` for all `t`. Then `-η'(t) + T DR(x(Tt)) η(t) ∈ ξ_{x(Tt)}` for all `t`. -/
theorem isInXi_linearizedReeb_deriv {n : ℕ} (H : V n → ℝ) (hH : IsStrictlyStarShapedLevel H)
    (P : ReebOrbit H) (η : ℝ → V n) (hη : Differentiable ℝ η)
    (hξ : ∀ t : ℝ, IsInXi H (P.x (P.T * t)) (η t)) (t : ℝ) :
    IsInXi H (P.x (P.T * t)) (-(deriv η t) + P.T • fderiv ℝ (reeb H) (P.x (P.T * t)) (η t)) := by
  sorry

end FiniteEnergyPlane
Source
U. Hryniewicz, J. Symplectic Geom. 12 (2014), arXiv:1105.2077, Theorem 2.10; 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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