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Trajectories on an ellipsoid rotate both complex planes

Proved
HryniewiczCriterion.ellipsoid_trajectory_rotation

by Mazecto · Oct 7, 2026 · Mathlib 0df444a (Lean v4.33.1)

dynamical-systemssymplectic-geometry

Let H(x)=q12+p12r12+q22+p22r22H(x)=\frac{q_1^2+p_1^2}{r_1^2}+\frac{q_2^2+p_2^2}{r_2^2}H(x)=r12​q12​+p12​​+r22​q22​+p22​​ on R4\mathbb R^4R4 with coordinates (q1,p1,q2,p2)(q_1,p_1,q_2,p_2)(q1​,p1​,q2​,p2​), and let yyy be a trajectory of XHX_HXH​ on {H=1}\{H=1\}{H=1} (convention ω0(XH,⋅)=−dH\omega_0(X_H,\cdot)=-dHω0​(XH​,⋅)=−dH). Then, writing zj=qj+ipjz_j=q_j+ip_jzj​=qj​+ipj​,

z1(t)=e2it/r12 z1(0),z2(t)=e2it/r22 z2(0).z_1(t)=e^{2it/r_1^2}\,z_1(0),\qquad z_2(t)=e^{2it/r_2^2}\,z_2(0).z1​(t)=e2it/r12​z1​(0),z2​(t)=e2it/r22​z2​(0).

The real and imaginary parts are written out in the Lean statement. No positivity of rjr_jrj​ is needed; for rj=0r_j=0rj​=0 both sides degenerate consistently with Lean's x/0=0x/0=0x/0=0.

Preamble
import Definitions.Def_HryniewiczCriterion_Basic
import Mathlib.Analysis.SpecialFunctions.Trigonometric.Basic
Formal statement
namespace HryniewiczCriterion

theorem ellipsoid_trajectory_rotation {r₁ r₂ : ℝ} {y : ℝ → R4}
    (hy : IsTrajectory (fun x : R4 => (x 0 ^ 2 + x 1 ^ 2) / r₁ ^ 2 + (x 2 ^ 2 + x 3 ^ 2) / r₂ ^ 2) y) (t : ℝ) :
    (y t 0 = Real.cos (2 / r₁ ^ 2 * t) * y 0 0 - Real.sin (2 / r₁ ^ 2 * t) * y 0 1 ∧
      y t 1 = Real.sin (2 / r₁ ^ 2 * t) * y 0 0 + Real.cos (2 / r₁ ^ 2 * t) * y 0 1) ∧
    (y t 2 = Real.cos (2 / r₂ ^ 2 * t) * y 0 2 - Real.sin (2 / r₂ ^ 2 * t) * y 0 3 ∧
      y t 3 = Real.sin (2 / r₂ ^ 2 * t) * y 0 2 + Real.cos (2 / r₂ ^ 2 * t) * y 0 3) := 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), https://arxiv.org/abs/1105.2077, p. 3 (ellipsoid example after Theorem 1.7)

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