Ambient rotation controls transverse winding up to 4pi
ProvedBirkhoffGlobalSection.ambient_rotation_transverse_bounddynamical-systemssymplectic-geometry
Let be a closed Hamiltonian solution of period for a smooth with nonzero differential along the orbit, with variational flow , and let be a continuous ambient determinant angle for . Then for every transverse tangent vector and every continuous polar angle of its transported quaternionic frame coordinates, the ambient increment over any period interval is controlled by the transverse increment up to :
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).