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Normalized winding profile and its angular derivative

Proved
HryniewiczCriterion.winding_endpoint_profile

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

differential-calculussymplectic-geometry

Let φ:[0,1]→SL(2,R)\varphi:[0,1]\to\mathrm{SL}(2,\mathbb R)φ:[0,1]→SL(2,R) be smooth and start at the identity. Put v(s)=(cos⁡s,sin⁡s)v(s)=(\cos s,\sin s)v(s)=(coss,sins) and let W(φ)W(\varphi)W(φ) be the set of normalized angular increments of the positive polar lifts initialized at s∈[0,2π]s\in[0,2\pi]s∈[0,2π]. There is a continuous function Δ:R→R\Delta:\mathbb R\to\mathbb RΔ:R→R such that

W(φ)=Δ([0,2π])=Δ(R).W(\varphi)=\Delta([0,2\pi])=\Delta(\mathbb R).W(φ)=Δ([0,2π])=Δ(R).

For every s∈Rs\in\mathbb Rs∈R there is a positive number rrr with

φ(1)v(s)=r v(s+2πΔ(s)),Δ′(s)=r−2−12π.\varphi(1)v(s)=r\,v(s+2\pi\Delta(s)),\qquad \Delta'(s)=\frac{r^{-2}-1}{2\pi}.φ(1)v(s)=rv(s+2πΔ(s)),Δ′(s)=2πr−2−1​.

The derivative is asserted at every real starting angle, including the angles representing the endpoints of the fundamental domain. This profile provides attained winding extrema and the derivative needed to detect fixed vectors at integer extrema. Formalization Note The path is represented on all real times but is constrained only on [0,1][0,1][0,1]; the winding set uses continuous positive polar lifts on that interval.

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

open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.winding_endpoint_profile
    (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) :
    ∃ Δ : ℝ → ℝ, Continuous Δ ∧
      windingInterval φ = Δ '' Set.Icc (0 : ℝ) (2 * Real.pi) ∧
      windingInterval φ = Set.range Δ ∧
      ∀ s : ℝ, ∃ r : ℝ, 0 < r ∧
        (φ 1).mulVec (rotationVector s) =
          r • rotationVector (s + 2 * Real.pi * Δ s) ∧
        HasDerivAt Δ ((1 / r ^ 2 - 1) / (2 * Real.pi)) s := 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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