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Solutions of the eigenvalue equation of the asymptotic operator on the line with prescribed initial value

Proved
FiniteEnergyPlane.exists_eigenEq_solution

by Mazecto · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

conley-zehnder-indexordinary-differential-equationssymplectic-geometry

Let S:R→R2n×2nS:\mathbb{R}\to\mathbb{R}^{2n\times2n}S:R→R2n×2n be continuous, J0=(0−IdId0)J_0=\begin{pmatrix}0&-\mathrm{Id}\\\mathrm{Id}&0\end{pmatrix}J0​=(0Id​−Id0​), μ∈R\mu\in\mathbb{R}μ∈R and v∈R2nv\in\mathbb{R}^{2n}v∈R2n. Then there is a differentiable x:R→R2nx:\mathbb{R}\to\mathbb{R}^{2n}x:R→R2n with x(0)=vx(0)=vx(0)=v and

−J0x′(t)−S(t)x(t)=μ x(t)for all t∈R.-J_0x'(t)-S(t)x(t)=\mu\,x(t)\qquad\text{for all }t\in\mathbb{R}.−J0​x′(t)−S(t)x(t)=μx(t)for all t∈R.

Global solvability of the initial value problem for the eigenvalue equation of the operator −J0∂t−S-J_0\partial_t-S−J0​∂t​−S on the whole line (no periodicity required); it provides the non-periodic solutions used to study the eigenvalues of the asymptotic operator.

Formalization Note R2n\mathbb{R}^{2n}R2n is CauchyRiemannIndex.Vec n and matrices are CauchyRiemannIndex.Mat n; J0J_0J0​ 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.

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