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A continuous angular displacement of a unipotent plane matrix has an integer extremum

Proved
HryniewiczCriterion.unipotent_rotation_profile_extremum

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

linear-algebrasymplectic-geometry

Let AAA be a real 2×22\times22×2 matrix satisfying det⁡A=1\det A=1detA=1 and det⁡(A−I)=0\det(A-I)=0det(A−I)=0. Let Δ:R→R\Delta:\mathbb R\to\mathbb RΔ:R→R be continuous and suppose that for every sss there is r>0r>0r>0 such that

A(cos⁡s,sin⁡s)=r (cos⁡(s+2πΔ(s)),sin⁡(s+2πΔ(s))).A(\cos s,\sin s)=r\,(\cos(s+2\pi\Delta(s)),\sin(s+2\pi\Delta(s))).A(coss,sins)=r(cos(s+2πΔ(s)),sin(s+2πΔ(s))).

Then some integer is an attained global minimum or an attained global maximum:

∃k∈Z,(k∈Δ(R) and ∀s, k≤Δ(s))or(k∈Δ(R) and ∀s, Δ(s)≤k).\exists k\in\mathbb Z,\quad \bigl(k\in\Delta(\mathbb R)\ \text{and}\ \forall s,\ k\le\Delta(s)\bigr) \quad\text{or}\quad \bigl(k\in\Delta(\mathbb R)\ \text{and}\ \forall s,\ \Delta(s)\le k\bigr).∃k∈Z,(k∈Δ(R) and ∀s, k≤Δ(s))or(k∈Δ(R) and ∀s, Δ(s)≤k).

This is the identity-or-shear part of the reverse implication of Hryniewicz's Lemma 2.1, stated solely in terms of the endpoint matrix and a continuous angular displacement, so it can be reused independently of a chosen path.

Preamble
import Definitions.Def_HryniewiczCriterion_ConleyZehnder
import Mathlib.Analysis.Calculus.Deriv.Basic

open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.unipotent_rotation_profile_extremum
    (A : Matrix (Fin 2) (Fin 2) ℝ) (hA : A.det = 1)
    (hdeg : (A - 1).det = 0) (Δ : ℝ → ℝ) (hΔ : Continuous Δ)
    (hpolar : ∀ s : ℝ, ∃ r : ℝ, 0 < r ∧
      A.mulVec (rotationVector s) = r • rotationVector (s + 2 * Real.pi * Δ s)) :
    ∃ k : ℤ, IsLeast (Set.range Δ) (k : ℝ) ∨
      IsGreatest (Set.range Δ) (k : ℝ) := by sorry
Source
Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, https://arxiv.org/abs/1105.2077, Section 2.1.1, pp. 5–6, angular description preceding Lemma 2.1 and its proof.

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