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Along a trajectory off the binding of a transverse disk open book, the page parameter is continuous and strictly monotone

Proved
HryniewiczCriterion.exists_page_parameter_along_trajectory

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

dynamical-systemsgeometry-topologysymplectic-geometry

Let yyy be a trajectory of XHX_HXH​ on SSS with y(0)∉x(R)y(0)\notin x(\mathbb{R})y(0)∈/x(R). Then yyy has a page parameter (Θ,u)(\Theta,u)(Θ,u) with Θ\ThetaΘ continuous and strictly monotone (strictly increasing or strictly decreasing): u(t)u(t)u(t) lies in the open unit disk and y(t)=pageΘ(t)(u(t))y(t)=\mathrm{page}_{\Theta(t)}(u(t))y(t)=pageΘ(t)​(u(t)) for every t∈Rt\in\mathbb{R}t∈R.

Here S=H−1(1)⊂R4S=H^{-1}(1)\subset\mathbb{R}^4S=H−1(1)⊂R4 is a strictly star-shaped level, P=(x,T)P=(x,T)P=(x,T) is a periodic orbit on SSS, and (pageθ)θ∈R(\mathrm{page}_\theta)_{\theta\in\mathbb{R}}(pageθ​)θ∈R​ is a transverse disk open book on SSS with binding PPP:

  • (θ,u)↦pageθ(u)(\theta,u)\mapsto\mathrm{page}_\theta(u)(θ,u)↦pageθ​(u) is C∞C^\inftyC∞ and 111-periodic in θ\thetaθ;
  • each pageθ\mathrm{page}_\thetapageθ​ restricts to a smooth embedding of the closed unit disk Dˉ\bar{\mathbb D}Dˉ into SSS (IsSmoothDiskEmbedding);
  • the boundary circle runs along PPP: pageθ(cos⁡2πt,sin⁡2πt)=x(Tt)\mathrm{page}_\theta(\cos2\pi t,\sin2\pi t)=x(Tt)pageθ​(cos2πt,sin2πt)=x(Tt);
  • XHX_HXH​ is transverse to every page in the interior: XH(pageθ(u))∉im⁡Dpageθ(u)X_H(\mathrm{page}_\theta(u))\notin\operatorname{im}D\mathrm{page}_\theta(u)XH​(pageθ​(u))∈/imDpageθ​(u) for ∣u∣<1|u|<1∣u∣<1;
  • (θ,u)↦pageθ(u)(\theta,u)\mapsto\mathrm{page}_\theta(u)(θ,u)↦pageθ​(u) maps [0,1)×D[0,1)\times\mathbb D[0,1)×D bijectively onto S∖x(R)S\setminus x(\mathbb{R})S∖x(R), with injective differential at every (θ,u)(\theta,u)(θ,u), ∣u∣<1|u|<1∣u∣<1.

These are exactly the open book hypotheses of isDiskLikeGlobalSectionMap_of_transverse_open_book.

A page parameter along a trajectory yyy of XHX_HXH​ on SSS is a pair of functions Θ:R→R\Theta:\mathbb{R}\to\mathbb{R}Θ:R→R, u:R→Du:\mathbb{R}\to\mathbb Du:R→D (open unit disk) with y(t)=pageΘ(t)(u(t))y(t)=\mathrm{page}_{\Theta(t)}(u(t))y(t)=pageΘ(t)​(u(t)) for all ttt.

Role: Θ\ThetaΘ is a real-valued lift, along the trajectory, of the angular coordinate S∖x(R)→R/ZS\setminus x(\mathbb{R})\to\mathbb{R}/\mathbb{Z}S∖x(R)→R/Z of the open book. No index hypothesis on PPP is needed.

Preamble
import Definitions.Def_HryniewiczCriterion_ConleyZehnder
import Definitions.Def_HryniewiczCriterion_GlobalSection
import Definitions.Def_HryniewiczCriterion_SelfLinking
import Mathlib.Topology.MetricSpace.HausdorffDistance
import Mathlib.Topology.Order.MonotoneConvergence

open HryniewiczCriterion
open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.exists_page_parameter_along_trajectory (H : R4 → ℝ)
    (hS : IsStrictlyStarShapedLevel H) (P : PeriodicOrbit H)
    (page : ℝ → Plane → R4)
    (hob : ContDiff ℝ ∞ (fun z : ℝ × Plane => page z.1 z.2) ∧
      (∀ θ u, page (θ + 1) u = page θ u) ∧
      (∀ θ, IsSmoothDiskEmbedding (page θ)) ∧
      (∀ θ, page θ '' closedUnitDisk ⊆ energySurface H) ∧
      (∀ θ t, page θ (circlePoint t) = P.x (P.T * t)) ∧
      (∀ θ, ∀ u ∈ openUnitDisk,
        hamiltonianVectorField H (page θ u) ∉ Set.range (fderiv ℝ (page θ) u)) ∧
      (∀ y ∈ energySurface H, y ∉ P.image →
        ∃! z : ℝ × Plane, z.1 ∈ Set.Ico (0 : ℝ) 1 ∧ z.2 ∈ openUnitDisk ∧ page z.1 z.2 = y) ∧
      (∀ θ : ℝ, ∀ u ∈ openUnitDisk,
        Function.Injective (fderiv ℝ (fun z : ℝ × Plane => page z.1 z.2) (θ, u))))
    (y : ℝ → R4) (hy : IsTrajectory H y) (hy0 : y 0 ∉ P.image) :
    ∃ (Θ : ℝ → ℝ) (u : ℝ → Plane), Continuous Θ ∧ (StrictMono Θ ∨ StrictAnti Θ) ∧
      ∀ t, u t ∈ openUnitDisk ∧ page (Θ t) (u t) = y t := by sorry
Source
cf. U. Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, J. Symplectic Geom. 12 (2014) 791-862, arXiv:1105.2077, Theorem 3.11 (p. 25); H. Hofer, K. Wysocki, E. Zehnder, The dynamics on three-dimensional strictly convex energy surfaces, Ann. of Math. 148 (1998) 197-289, Theorem 2.5.

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