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Polar-angle criterion for winding above one in SL(2,R)SL(2,\mathbb{R})SL(2,R)

Proved
HryniewiczCriterion.polar_angle_windingInterval_gt_one

by Mazecto · Oct 6, 2026 · Mathlib 0df444a (Lean v4.33.1)

contact-geometryhamiltonian-dynamicssymplectic-geometry

Let φ:[0,1]→SL(2,R)\varphi:[0,1]\to SL(2,\mathbb{R})φ:[0,1]→SL(2,R) be smooth with φ(0)=I\varphi(0)=Iφ(0)=I, and let α\alphaα be its continuous polar angle: φ(t)=R(α(t))P(t)\varphi(t)=R(\alpha(t))P(t)φ(t)=R(α(t))P(t) with P(t)P(t)P(t) symmetric positive definite and α(0)=0\alpha(0)=0α(0)=0. Let λ1,λ2\lambda_1,\lambda_2λ1​,λ2​ be the eigenvalues of the graph unitary W(Γφ(1))W(Δ)−1W(\Gamma_{\varphi(1)})W(\Delta)^{-1}W(Γφ(1)​)W(Δ)−1 in (R2⊕R2,−ω0⊕ω0)(\mathbb{R}^2\oplus\mathbb{R}^2,-\omega_0\oplus\omega_0)(R2⊕R2,−ω0​⊕ω0​), and ang⁡(λ)∈(0,2π]\operatorname{ang}(\lambda)\in(0,2\pi]ang(λ)∈(0,2π] their arguments with ang⁡(1)=2π\operatorname{ang}(1)=2\piang(1)=2π. If

2 α(1)  ≥  4π+ang⁡(λ1)+ang⁡(λ2),2\,\alpha(1)\;\ge\;4\pi+\operatorname{ang}(\lambda_1)+\operatorname{ang}(\lambda_2),2α(1)≥4π+ang(λ1​)+ang(λ2​),

then every vector turns strictly more than once under φ\varphiφ: the winding interval I(φ)I(\varphi)I(φ) lies in (1,∞)(1,\infty)(1,∞).

This is the two-dimensional index computation behind HWZ (3.45)–(3.46), in the lower semicontinuous convention of Hryniewicz (5): it converts a bound on the polar angle of the contact path into the winding bound that characterizes Conley–Zehnder index at least three.

Preamble
import Definitions.Def_HryniewiczCriterion_GraphAngle

open HryniewiczCriterion
open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.polar_angle_windingInterval_gt_one (φ : ℝ → Matrix (Fin 2) (Fin 2) ℝ)
    (hφ : ContDiffOn ℝ ∞ (fun t i j => φ t i j) (Set.Icc 0 1))
    (hsymp : ∀ t ∈ Set.Icc (0 : ℝ) 1, (φ t).det = 1) (h0 : φ 0 = 1)
    (α : ℝ → ℝ) (hα : IsPolarAngleLift φ α)
    (h : 4 * Real.pi + eigenAngleSum (graphUnitary2 (φ 1)) ≤ 2 * α 1) :
    ∀ d ∈ windingInterval φ, 1 < d := by sorry
Source
Hofer–Wysocki–Zehnder, The dynamics on three-dimensional strictly convex energy surfaces, Ann. of Math. 148 (1998), https://doi.org/10.2307/120994, proof of Theorem 3.4, (3.45)–(3.46), p. 222, in the winding-interval form of Hryniewicz, https://arxiv.org/html/1105.2077v5, Section 2.1.1, equations (4)–(5). Reduction lemma; not a verbatim numbered assertion.

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