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Ambient rotation controls transverse winding up to 4pi

Proved
BirkhoffGlobalSection.ambient_rotation_transverse_bound

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

dynamical-systemssymplectic-geometry

Let xxx be a closed Hamiltonian solution of period TTT for a smooth FFF with nonzero differential along the orbit, with variational flow YYY, and let α\alphaα be a continuous ambient determinant angle for YYY. Then for every transverse tangent vector vvv and every continuous polar angle θ\thetaθ of its transported quaternionic frame coordinates, the ambient increment over any period interval is controlled by the transverse increment up to 4π4\pi4π:

α(a+T)−α(a)≤θ(T)−θ(0)+4πfor every a.\alpha(a+T)-\alpha(a) \le \theta(T)-\theta(0)+4\pi \qquad\text{for every }a.α(a+T)−α(a)≤θ(T)−θ(0)+4πfor every a.

Reducing the ambient rotation to the transverse frame costs at most one full turn, and moving the start of the period interval costs another; both errors are uniform in the vector, the angle, and the starting time. No nondegeneracy or least-period assumption is needed.

Preamble
import Definitions.Def_BirkhoffGlobalSection_AmbientRotation

open scoped ContDiff
Formal statement
namespace BirkhoffGlobalSection

open scoped ContDiff

theorem ambient_rotation_transverse_bound
    (F : Phase → ℝ) (S : Set Phase) (x : ℝ → Phase) (T : ℝ)
    (hx : IsPeriodicHamiltonianSolutionIn F S x T)
    (hregular : ∀ t : ℝ, ContDiffAt ℝ ∞ F (x t) ∧ fderiv ℝ F (x t) ≠ 0)
    (Y : ℝ → (Phase →L[ℝ] Phase))
    (hY : IsHamiltonianVariationalSolution F x Y)
    (α : ℝ → ℝ) (hα : IsAmbientRotationAngle Y α) :
    ∀ v : Phase, fderiv ℝ F (x 0) v = 0 →
      transverseFrameCoordinates (TangentialHessian.grad F (x 0)) v ≠ 0 →
      ∀ θ : ℝ → ℝ, Continuous θ →
        (∀ t : ℝ, ∃ ρ : ℝ, 0 < ρ ∧
          transverseFrameCoordinates (TangentialHessian.grad F (x t)) (Y t v) =
            ![ρ * Real.cos (θ t), ρ * Real.sin (θ t)]) →
        ∀ a : ℝ, α (a + T) - α a ≤ θ T - θ 0 + 4 * Real.pi := by sorry

end BirkhoffGlobalSection
Source
Auxiliary consequence of the quaternionic frame and reduced variational flow in Joung-van Koert, https://arxiv.org/html/2407.19159v3, Section 2.3, and the complex-linear determinant rotation map in Gutt, https://arxiv.org/pdf/1307.7239, p. 2, Theorem 1, Eq. (3).

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