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Linear ambient-angle growth from the spectral splitting

Proved
BirkhoffGlobalSection.saddle_center_angle_linear_growth

by caleb · Sep 28, 2026 · Mathlib 0df444a (Lean v4.33.1)

dynamical-systemssymplectic-geometry

From the spectral splitting, the ambient determinant angle grows at a uniform linear rate. The elliptic plane forces steady rotation while the hyperbolic directions contribute only a bounded wobble, so for fixed rate c0>0c_0>0c0​>0 and constant C0C_0C0​, on every interval [a,a+L][a,a+L][a,a+L] the fundamental solution admits a continuous ambient angle with

α0(a+L)−α0(a)>c0L−C0.\alpha_0(a+L)-\alpha_0(a) > c_0 L - C_0.α0​(a+L)−α0​(a)>c0​L−C0​.

This is the quantitative core of the rotation mechanism: it turns the algebraic splitting into the uniform estimate from which unboundedness follows by pure logic. The constants depend only on the splitting data.

Preamble
import Definitions.Def_BirkhoffGlobalSection_AmbientRotation
Formal statement
namespace BirkhoffGlobalSection

theorem saddle_center_angle_linear_growth
    (ω lam : ℝ) (hω : 0 < ω) (hlam : 0 < lam)
    (e₁ e₂ f₁ f₂ : Phase)
    (he₁ : TangentialHessian.qI.mulVec
        (((!![-16, 0, 0, 1; 0, 8, -1, 0; 0, -1, 1, 0; 1, 0, 0, 1] :
          Matrix (Fin 4) (Fin 4) ℝ).mulVec e₁)) = ω • e₂)
    (he₂ : TangentialHessian.qI.mulVec
        (((!![-16, 0, 0, 1; 0, 8, -1, 0; 0, -1, 1, 0; 1, 0, 0, 1] :
          Matrix (Fin 4) (Fin 4) ℝ).mulVec e₂)) = -ω • e₁)
    (hf₁ : TangentialHessian.qI.mulVec
        (((!![-16, 0, 0, 1; 0, 8, -1, 0; 0, -1, 1, 0; 1, 0, 0, 1] :
          Matrix (Fin 4) (Fin 4) ℝ).mulVec f₁)) = lam • f₁)
    (hf₂ : TangentialHessian.qI.mulVec
        (((!![-16, 0, 0, 1; 0, 8, -1, 0; 0, -1, 1, 0; 1, 0, 0, 1] :
          Matrix (Fin 4) (Fin 4) ℝ).mulVec f₂)) = -lam • f₂)
    (hindep : LinearIndependent ℝ ![e₁, e₂, f₁, f₂]) :
    ∃ c₀ : ℝ, 0 < c₀ ∧ ∃ C₀ : ℝ, ∀ a L : ℝ,
      ∃ (Φ0 : ℝ → (Phase →L[ℝ] Phase)) (α0 : ℝ → ℝ),
        Φ0 a = ContinuousLinearMap.id ℝ Phase ∧
        (∀ t ∈ Set.Icc a (a + L), ∀ v : Phase,
          HasDerivAt (fun τ => Φ0 τ v)
            (TangentialHessian.qI.mulVec
              ((!![-16, 0, 0, 1; 0, 8, -1, 0; 0, -1, 1, 0; 1, 0, 0, 1] :
                Matrix (Fin 4) (Fin 4) ℝ).mulVec (Φ0 t v))) t) ∧
        ContinuousOn α0 (Set.Icc a (a + L)) ∧
        (∀ t ∈ Set.Icc a (a + L), ∃ ρ : ℝ, 0 < ρ ∧
          ambientRotationDet (Φ0 t) = ⟨ρ * Real.cos (α0 t), ρ * Real.sin (α0 t)⟩) ∧
        c₀ * L - C₀ < α0 (a + L) - α0 a := by sorry

end BirkhoffGlobalSection
Source
Liu--Salomao, https://arxiv.org/html/2506.17867v2#S7, Eq. (7.7) and the proof of Theorem 1.8 (the linearized flow at the saddle-center splits into a hyperbolic and an elliptic part, and the elliptic part forces index growth). Gutt, https://arxiv.org/pdf/1307.7239, Eq. (9). H0 is the Hessian of the platform Levi-Civita Hamiltonian at mu = 1/2, c = 2.

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