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A continuous path in SL(2,R)SL(2,\mathbb{R})SL(2,R) has a continuous polar angle

Proved
HryniewiczCriterion.exists_polarAngleLift

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

hamiltonian-dynamicssymplectic-geometry

Let φ:[0,1]→SL(2,R)\varphi:[0,1]\to SL(2,\mathbb{R})φ:[0,1]→SL(2,R) be continuous with φ(0)=I\varphi(0)=Iφ(0)=I. Then there is a continuous function α:[0,1]→R\alpha:[0,1]\to\mathbb{R}α:[0,1]→R with α(0)=0\alpha(0)=0α(0)=0 such that

φ(t)=R(α(t)) P(t)(t∈[0,1]),\varphi(t)=R(\alpha(t))\,P(t)\qquad(t\in[0,1]),φ(t)=R(α(t))P(t)(t∈[0,1]),

where R(α)R(\alpha)R(α) is the rotation by α\alphaα and each P(t)P(t)P(t) is symmetric positive definite.

The function α\alphaα is the continuous rotation angle in the polar decomposition of the path. Its endpoint value α(1)\alpha(1)α(1) measures the total rotation of φ\varphiφ and is the quantity compared with winding numbers in Conley–Zehnder index estimates.

Preamble
import Definitions.Def_HryniewiczCriterion_GraphAngle

open HryniewiczCriterion
open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.exists_polarAngleLift (φ : ℝ → Matrix (Fin 2) (Fin 2) ℝ)
    (hc : ContinuousOn (fun t i j => φ t i j) (Set.Icc 0 1))
    (hdet : ∀ t ∈ Set.Icc (0 : ℝ) 1, (φ t).det = 1) (h0 : φ 0 = 1) :
    ∃ α : ℝ → ℝ, IsPolarAngleLift φ α := by sorry
Source
Standard (polar decomposition in SL(2,R)SL(2,\mathbb{R})SL(2,R)); used for the rotation angle of the linearized flow in Hofer–Wysocki–Zehnder, The dynamics on three-dimensional strictly convex energy surfaces, Ann. of Math. 148 (1998), https://doi.org/10.2307/120994, pp. 221–222.

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