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Each winding number belongs to a two-dimensional space of eigenfunctions

Proved
FiniteEnergyPlane.loopEigenSpan_finrank_eq_two

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

conley-zehnder-indexpseudoholomorphic-curvesreeb-dynamicssymplectic-geometrysymplectizationwinding-numbers

Let S∞:R→R2×2S_\infty:\mathbb{R}\to\mathbb{R}^{2\times2}S∞​:R→R2×2 be a C∞C^\inftyC∞ 111-periodic loop of symmetric matrices and A=−J0∂t−S∞A=-J_0\partial_t-S_\inftyA=−J0​∂t​−S∞​ on 111-periodic loops in R2=C\mathbb{R}^2=\mathbb{C}R2=C. For every k∈Zk\in\mathbb{Z}k∈Z, the eigenfunctions of AAA whose eigenvalue has winding kkk span a real vector space of dimension exactly 222.

Formalization Note The span is loopEigenSpan Sinf k, a submodule of ℝ → CauchyRiemannIndex.Vec 1; the statement includes FiniteDimensional, so Module.finrank is the actual dimension.

Preamble
import Definitions.Def_FiniteEnergyPlane_Winding
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Wendl, Theorem 3.7.1 (4): for every `k ∈ ℤ`, the eigenfunctions of `A = -J₀ ∂ₜ - S∞` with
winding number `k` span a real vector space of dimension exactly `2`. In particular every
winding number is attained, by one eigenvalue of multiplicity `2` or by two eigenvalues of
multiplicity `1`. -/
theorem loopEigenSpan_finrank_eq_two (Sinf : ℝ → CauchyRiemannIndex.Mat 1) (hSinf : CauchyRiemannIndex.IsSymLoop Sinf)
    (hSinf' : ∀ i j, ContDiff ℝ ∞ (fun t => Sinf t i j)) (k : ℤ) :
    FiniteDimensional ℝ (loopEigenSpan Sinf k) ∧ Module.finrank ℝ (loopEigenSpan Sinf k) = 2 := by
  sorry

end FiniteEnergyPlane
Source
C. Wendl, Lectures on Symplectic Field Theory, lecture notes, Humboldt-Universität zu Berlin (2026 version); earlier version arXiv:1612.01009, Theorem 3.7.1 (4); H. Hofer, K. Wysocki, E. Zehnder, Properties of pseudoholomorphic curves in symplectisations II: Embedding controls and algebraic invariants, Geom. Funct. Anal. 5 (1995), 270–328, Section 3
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What the Lean code literally says, in plain math · claude-opus-5-5

Theorem FiniteEnergyPlane.loopEigenSpan_finrank_eq_two

Let S∞:R→R2×2S_\infty : \mathbb{R} \to \mathbb{R}^{2\times 2}S∞​:R→R2×2 be a loop of real 2×22\times 22×2 matrices (indices "left", "right") that is continuous, 111-periodic, symmetric at every ttt, and has C∞C^\inftyC∞ entries t↦S∞(t)ijt \mapsto S_\infty(t)_{ij}t↦S∞​(t)ij​. Let k∈Zk \in \mathbb{Z}k∈Z be arbitrary.

Consider the real vector space of all functions R→R2\mathbb{R} \to \mathbb{R}^2R→R2, and in it the subspace

Ek=span⁡R{ e  :  ∃μ∈R, e is a loop eigenfunction for (S∞,μ) and HasLoopEigenWind(S∞,μ,k) }.E_k = \operatorname{span}_{\mathbb{R}}\big\{\, e \;:\; \exists \mu \in \mathbb{R},\ e \text{ is a loop eigenfunction for } (S_\infty,\mu) \text{ and } \mathrm{HasLoopEigenWind}(S_\infty, \mu, k) \,\big\}.Ek​=spanR​{e:∃μ∈R, e is a loop eigenfunction for (S∞​,μ) and HasLoopEigenWind(S∞​,μ,k)}.

Here a loop eigenfunction for (S∞,μ)(S_\infty,\mu)(S∞​,μ) is a C∞C^\inftyC∞, 111-periodic e:R→R2e : \mathbb{R}\to\mathbb{R}^2e:R→R2, not identically zero, with

−J0 e′(t)−S∞(t) e(t)=μ e(t)  for all t,J0=(0−110);-J_0\, e'(t) - S_\infty(t)\, e(t) = \mu\, e(t)\ \ \text{for all } t, \qquad J_0 = \begin{pmatrix} 0 & -1 \\ 1 & 0 \end{pmatrix};−J0​e′(t)−S∞​(t)e(t)=μe(t)  for all t,J0​=(01​−10​);

and HasLoopEigenWind(S∞,μ,k)\mathrm{HasLoopEigenWind}(S_\infty, \mu, k)HasLoopEigenWind(S∞​,μ,k) means that μ\muμ has at least one loop eigenfunction and every loop eigenfunction eee of μ\muμ has winding number kkk, i.e. f(t)=eL(t)+i eR(t)f(t) = e_L(t) + i\,e_R(t)f(t)=eL​(t)+ieR​(t) is continuous, 111-periodic, nowhere zero, with a continuous argument θ\thetaθ (f=∣f∣eiθf = |f| e^{i\theta}f=∣f∣eiθ) satisfying θ(1)−θ(0)=2πk\theta(1) - \theta(0) = 2\pi kθ(1)−θ(0)=2πk.

The theorem asserts that EkE_kEk​ is finite-dimensional over R\mathbb{R}R and

dim⁡REk=2.\dim_{\mathbb{R}} E_k = 2.dimR​Ek​=2.

Since kkk ranges over all integers with no further hypothesis, this claims in particular that for every integer kkk (positive, zero or negative) the set of eigenvalues all of whose eigenfunctions wind exactly kkk times is non-empty, and the eigenfunctions of all such eigenvalues together span exactly a 2-dimensional space.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Mazecto · Nov 1, 2026

    Confirmed by the mission captain (proposal self-audit).

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