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Ellipsoids: both axes bind adapted open books with disk-like pages

Proved
HryniewiczCriterion.ellipsoid_axes_bind_adapted_open_books

by Mazecto · Oct 5, 2026 · Mathlib 0df444a (Lean v4.33.1)

contact-geometrydynamical-systemssymplectic-geometry

Let r1,r2>0r_1,r_2>0r1​,r2​>0 and let SSS be the boundary of the ellipsoid

q12+p12r12+q22+p22r22=1.\frac{q_1^2+p_1^2}{r_1^2}+\frac{q_2^2+p_2^2}{r_2^2}=1.r12​q12​+p12​​+r22​q22​+p22​​=1.

Let PPP be a prime periodic orbit of XHX_HXH​ on SSS, with HHH the left-hand side, whose image lies in one of the two axes {q2=p2=0}\{q_2=p_2=0\}{q2​=p2​=0} or {q1=p1=0}\{q_1=p_1=0\}{q1​=p1​=0}. Then PPP is the binding of an open book decomposition of SSS with disk-like pages that is adapted to the flow: every page is a disk-like global surface of section with oriented boundary PPP.

Hryniewicz notes that the axes of an ellipsoid are bindings of adapted open books, while the Hofer–Wysocki–Zehnder theorem detects only the axis of smaller action. The statement is an explicit example of the notions used in Theorems 1.7 and 1.8. It checks that the definitions of global sections and open books are satisfiable.

Preamble
import Definitions.Def_HryniewiczCriterion_GlobalSection
Formal statement
namespace HryniewiczCriterion

/-- Hryniewicz, p. 3: on the boundary of an ellipsoid, each of the two axis circles is
the binding of an adapted open book decomposition with disk-like pages. -/
theorem ellipsoid_axes_bind_adapted_open_books (r₁ r₂ : ℝ) (h₁ : 0 < r₁) (h₂ : 0 < r₂)
    (P : PeriodicOrbit
      (fun x : R4 => (x 0 ^ 2 + x 1 ^ 2) / r₁ ^ 2 + (x 2 ^ 2 + x 3 ^ 2) / r₂ ^ 2))
    (hP : P.IsPrime)
    (haxis : P.image ⊆ {x | x 2 = 0 ∧ x 3 = 0} ∨ P.image ⊆ {x | x 0 = 0 ∧ x 1 = 0}) :
    HasAdaptedDiskOpenBook
      (fun x : R4 => (x 0 ^ 2 + x 1 ^ 2) / r₁ ^ 2 + (x 2 ^ 2 + x 3 ^ 2) / r₂ ^ 2) P := by sorry

end HryniewiczCriterion
Source
Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, J. Symplectic Geom. 12 (2014) 791-862, https://arxiv.org/abs/1105.2077, p. 3, paragraph after Theorem 1.7
Read-back

What the Lean code literally says, in plain math · claude-opus-5-5

Read-back. Let r1,r2r_1, r_2r1​,r2​ be real numbers with r1>0r_1 > 0r1​>0 and r2>0r_2 > 0r2​>0 (equality r1=r2r_1 = r_2r1​=r2​ is allowed). Coordinates on R4\mathbb{R}^4R4 are x=(x0,x1,x2,x3)x = (x_0,x_1,x_2,x_3)x=(x0​,x1​,x2​,x3​) and the Hamiltonian is the fixed quadratic

H(x)=x02+x12r12+x22+x32r22,Σ={x:H(x)=1}.H(x) = \frac{x_0^2 + x_1^2}{r_1^2} + \frac{x_2^2 + x_3^2}{r_2^2}, \qquad \Sigma = \{x : H(x) = 1\}.H(x)=r12​x02​+x12​​+r22​x22​+x32​​,Σ={x:H(x)=1}.

The Hamiltonian vector field is XH(x)=(−∂1H,∂0H,−∂3H,∂2H)(x)X_H(x) = (-\partial_1 H, \partial_0 H, -\partial_3 H, \partial_2 H)(x)XH​(x)=(−∂1​H,∂0​H,−∂3​H,∂2​H)(x), here XH(x)=(−2x1/r12, 2x0/r12, −2x3/r22, 2x2/r22)X_H(x) = \bigl(-2x_1/r_1^2,\ 2x_0/r_1^2,\ -2x_3/r_2^2,\ 2x_2/r_2^2\bigr)XH​(x)=(−2x1​/r12​, 2x0​/r12​, −2x3​/r22​, 2x2​/r22​). A trajectory is a curve y:R→R4y:\mathbb{R}\to\mathbb{R}^4y:R→R4 with y′(t)=XH(y(t))y'(t) = X_H(y(t))y′(t)=XH​(y(t)) and H(y(t))=1H(y(t)) = 1H(y(t))=1 for all t∈Rt \in \mathbb{R}t∈R.

Hypotheses on the orbit.

  • PPP is a periodic orbit: a trajectory x:R→R4x : \mathbb{R} \to \mathbb{R}^4x:R→R4 together with a real T>0T > 0T>0 such that x(t+T)=x(t)x(t + T) = x(t)x(t+T)=x(t) for all ttt.
  • (prime) x(t)≠x(0)x(t) \neq x(0)x(t)=x(0) for every 0<t<T0 < t < T0<t<T.
  • (axis) the image x(R)x(\mathbb{R})x(R) lies in the plane {x2=x3=0}\{x_2 = x_3 = 0\}{x2​=x3​=0}, or it lies in the plane {x0=x1=0}\{x_0 = x_1 = 0\}{x0​=x1​=0}.

Conclusion. There exists a family p:R×R2→R4p : \mathbb{R} \times \mathbb{R}^2 \to \mathbb{R}^4p:R×R2→R4, written pθ(u)p_\theta(u)pθ​(u), with all of the following properties. Here D={u02+u12≤1}D = \{u_0^2+u_1^2 \le 1\}D={u02​+u12​≤1} is the closed unit disk, D˚={u02+u12<1}\mathring D = \{u_0^2+u_1^2 < 1\}D˚={u02​+u12​<1} the open disk, S1={u02+u12=1}S^1 = \{u_0^2+u_1^2 = 1\}S1={u02​+u12​=1} the unit circle, and ω0(a,b)=a0b1−a1b0+a2b3−a3b2\omega_0(a,b) = a_0b_1 - a_1b_0 + a_2b_3 - a_3b_2ω0​(a,b)=a0​b1​−a1​b0​+a2​b3​−a3​b2​.

  1. Smooth: (θ,u)↦pθ(u)(\theta, u) \mapsto p_\theta(u)(θ,u)↦pθ​(u) is C∞C^\inftyC∞ on all of R×R2\mathbb{R} \times \mathbb{R}^2R×R2.
  2. Periodic in θ\thetaθ: pθ+1(u)=pθ(u)p_{\theta+1}(u) = p_\theta(u)pθ+1​(u)=pθ​(u) for all θ,u\theta, uθ,u.
  3. Each page is a disk-like global section for PPP: for every θ\thetaθ, the map e=pθe = p_\thetae=pθ​ satisfies
    • eee is C∞C^\inftyC∞ on R2\mathbb{R}^2R2, injective on DDD, and its derivative De(u)De(u)De(u) is injective for every u∈Du \in Du∈D;
    • e(D)⊆Σe(D) \subseteq \Sigmae(D)⊆Σ;
    • e(S1)=x(R)e(S^1) = x(\mathbb{R})e(S1)=x(R) (equality of sets);
    • for every u∈D˚u \in \mathring Du∈D˚, XH(e(u))X_H(e(u))XH​(e(u)) is not in the image of De(u)De(u)De(u);
    • for every trajectory yyy with y(0)∉x(R)y(0) \notin x(\mathbb{R})y(0)∈/x(R) and every a∈Ra \in \mathbb{R}a∈R, there exist t>at > at>a with y(t)∈e(D)y(t) \in e(D)y(t)∈e(D) and t′<at' < at′<a with y(t′)∈e(D)y(t') \in e(D)y(t′)∈e(D) (the trajectory meets the image of the closed disk at arbitrarily late and arbitrarily early times).
  4. Common binding, parametrized by the orbit: for all θ,t∈R\theta, t \in \mathbb{R}θ,t∈R,
pθ(cos⁡2πt, sin⁡2πt)=x(Tt).p_\theta(\cos 2\pi t,\ \sin 2\pi t) = x(Tt).pθ​(cos2πt, sin2πt)=x(Tt).
  1. Positivity: for all θ\thetaθ and u∈D˚u \in \mathring Du∈D˚,
ω0(∂u0pθ(u), ∂u1pθ(u))>0.\omega_0\bigl(\partial_{u_0} p_\theta(u),\ \partial_{u_1} p_\theta(u)\bigr) > 0.ω0​(∂u0​​pθ​(u), ∂u1​​pθ​(u))>0.
  1. Fibration: for every y∈Σy \in \Sigmay∈Σ with y∉x(R)y \notin x(\mathbb{R})y∈/x(R) there is exactly one pair (θ,u)(\theta, u)(θ,u) with θ∈[0,1)\theta \in [0,1)θ∈[0,1), u∈D˚u \in \mathring Du∈D˚ and pθ(u)=yp_\theta(u) = ypθ​(u)=y.
  2. Regularity: for every θ∈R\theta \in \mathbb{R}θ∈R and u∈D˚u \in \mathring Du∈D˚, the derivative of (θ,u)↦pθ(u)(\theta,u)\mapsto p_\theta(u)(θ,u)↦pθ​(u) at (θ,u)(\theta,u)(θ,u), a linear map R×R2→R4\mathbb{R}\times\mathbb{R}^2 \to \mathbb{R}^4R×R2→R4, is injective.

Edge cases. The theorem is stated for the given parametrization xxx of PPP (including its starting point x(0)x(0)x(0) and period TTT); property 4 ties all pages to that parametrization. The primality hypothesis makes TTT the minimal positive time of return to x(0)x(0)x(0). The axis hypothesis is a disjunction; nothing further about which plane is required. No statement is made about pages for θ\thetaθ beyond what periodicity and properties 3–7 give.

Human review
  • Endorsed by Shuze Chen · Oct 6, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Mazecto · Oct 6, 2026

    Confirmed by the mission captain (proposal self-audit).

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