Solutions of the eigenvalue equation of the asymptotic operator on the line with prescribed initial value
ProvedFiniteEnergyPlane.exists_eigenEq_solutionconley-zehnder-indexordinary-differential-equationssymplectic-geometry
Let be continuous, , and . Then there is a differentiable with and
Global solvability of the initial value problem for the eigenvalue equation of the operator on the whole line (no periodicity required); it provides the non-periodic solutions used to study the eigenvalues of the asymptotic operator.
Formalization Note is CauchyRiemannIndex.Vec n and matrices are CauchyRiemannIndex.Mat n; is CauchyRiemannIndex.J₀ n and matrices act through Matrix.toEuclideanLin; the derivative is deriv x t together with Differentiable ℝ x.
Preamble
import Definitions.Def_FiniteEnergyPlane_Winding
Formal statement
namespace FiniteEnergyPlane
/-- For continuous `S : ℝ → ℝ^{2n×2n}`, `μ ∈ ℝ` and `v ∈ ℝ^{2n}`, the equation
`-J₀ x' - S x = μ x` has a differentiable solution `x : ℝ → ℝ^{2n}` on all of `ℝ` with
`x 0 = v`. -/
theorem exists_eigenEq_solution {n : ℕ} (S : ℝ → CauchyRiemannIndex.Mat n) (hS : Continuous S)
(μ : ℝ) (v : CauchyRiemannIndex.Vec n) :
∃ x : ℝ → CauchyRiemannIndex.Vec n, x 0 = v ∧ Differentiable ℝ x ∧
∀ t, -(Matrix.toEuclideanLin (CauchyRiemannIndex.J₀ n) (deriv x t)) -
Matrix.toEuclideanLin (S t) (x t) = μ • x t := by
sorry
end FiniteEnergyPlane
Source
C. Wendl, Lectures on Symplectic Field Theory (2026 notes), arXiv:1612.01009, Sections 3.4 and 3.7; standard linear ODE theory.