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Eigenvalues of the graph unitary of R(x)PR(x)PR(x)P in Sp(1)\mathrm{Sp}(1)Sp(1)

Proved
HryniewiczCriterion.graphUnitary2_polar_roots

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

linear-algebrasymplectic-geometry

Let PPP be a real symmetric positive definite 2×22\times22×2 matrix with det⁡P=1\det P=1detP=1, let x∈Rx\in\mathbb{R}x∈R, and let g=R(x)P∈SL(2,R)g=R(x)P\in SL(2,\mathbb{R})g=R(x)P∈SL(2,R) (every element of SL(2,R)SL(2,\mathbb{R})SL(2,R) has this polar form). Put γ=arccos⁡(2/tr⁡P)∈[0,π/2)\gamma=\arccos(2/\operatorname{tr}P)\in[0,\pi/2)γ=arccos(2/trP)∈[0,π/2). Then the eigenvalues of the graph unitary W(Γg)W(Δ)−1W(\Gamma_g)W(\Delta)^{-1}W(Γg​)W(Δ)−1 (Souriau map of the graph Γg⊂(R2⊕R2,−ω0⊕ω0)\Gamma_g\subset(\mathbb{R}^2\oplus\mathbb{R}^2,-\omega_0\oplus\omega_0)Γg​⊂(R2⊕R2,−ω0​⊕ω0​), Δ\DeltaΔ the diagonal) are

ei(x+γ),ei(x−γ),e^{i(x+\gamma)},\qquad e^{i(x-\gamma)},ei(x+γ),ei(x−γ),

counted with multiplicity. In particular the rotation part of ggg is the mean of the two eigen-angles, and the half-gap γ\gammaγ depends only on tr⁡P\operatorname{tr}PtrP.

Preamble
import Definitions.Def_HryniewiczCriterion_GraphAngle

open HryniewiczCriterion
open scoped ContDiff
Formal statement
theorem HryniewiczCriterion.graphUnitary2_polar_roots (x : ℝ) {P : Matrix (Fin 2) (Fin 2) ℝ} (hP : P.PosDef)
    (hdet : P.det = 1) :
    (graphUnitary2 (rotationMatrix x * P)).charpoly.roots =
      {Complex.exp ((x + Real.arccos (2 / (P 0 0 + P 1 1))) * Complex.I),
        Complex.exp ((x - Real.arccos (2 / (P 0 0 + P 1 1))) * Complex.I)} := 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, the eigenvalue computation behind (3.45)–(3.46), p. 222; Souriau map as in Robbin–Salamon, The Maslov index for paths, Topology 32 (1993). Explicit formula; not a verbatim numbered assertion.

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