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Derivative of the cross term of two eigenfunctions of the asymptotic operator

Proved
FiniteEnergyPlane.hasDerivAt_im_conj_mul_loopEigen

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

conley-zehnder-indexpseudoholomorphic-curvessymplectic-geometrywinding-numbers

Let S∞:R→R2×2S_\infty:\mathbb{R}\to\mathbb{R}^{2\times2}S∞​:R→R2×2 be a continuous 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. Let e1,e2e_1,e_2e1​,e2​ be eigenfunctions of AAA with eigenvalues μ1,μ2\mu_1,\mu_2μ1​,μ2​, viewed as loops f1,f2f_1,f_2f1​,f2​ in C\mathbb{C}C. Then for every ttt,

ddtIm⁡(f1(t)‾ f2(t))=(μ2−μ1)Re⁡(f1(t)‾ f2(t)).\frac{d}{dt}\operatorname{Im}\big(\overline{f_1(t)}\,f_2(t)\big)=(\mu_2-\mu_1)\operatorname{Re}\big(\overline{f_1(t)}\,f_2(t)\big).dtd​Im(f1​(t)​f2​(t))=(μ2​−μ1​)Re(f1​(t)​f2​(t)).

An exact differential identity for pairs of eigenfunctions of the asymptotic operator, used to compare their winding numbers.

Formalization Note Eigenfunctions are IsLoopEigen Sinf μ e (FiniteEnergyPlane_Asymptotics: smooth, 111-periodic, not identically zero, −J0e′−S∞e=μe-J_0e'-S_\infty e=\mu e−J0​e′−S∞​e=μe); symmetry and continuity are CauchyRiemannIndex.IsSymLoop Sinf; fjf_jfj​ is fun t => vecToC (e_j t) and the conclusion is a HasDerivAt statement at every t.

Preamble
import Definitions.Def_FiniteEnergyPlane_Winding
Formal statement
namespace FiniteEnergyPlane

/-- For eigenfunctions `e₁, e₂` of `A = -J₀ ∂ₜ - S∞` (symmetric `S∞`) with eigenvalues `μ₁, μ₂`,
read as loops `f₁, f₂` in `ℂ`, the imaginary part of `conj f₁ · f₂` has derivative
`(μ₂ - μ₁) Re(conj f₁ · f₂)`. -/
theorem hasDerivAt_im_conj_mul_loopEigen (Sinf : ℝ → CauchyRiemannIndex.Mat 1)
    (hSinf : CauchyRiemannIndex.IsSymLoop Sinf) {μ₁ μ₂ : ℝ}
    {e₁ e₂ : ℝ → CauchyRiemannIndex.Vec 1} (h₁ : IsLoopEigen Sinf μ₁ e₁)
    (h₂ : IsLoopEigen Sinf μ₂ e₂) (t : ℝ) :
    HasDerivAt (fun s => (starRingEnd ℂ (vecToC (e₁ s)) * vecToC (e₂ s)).im)
      ((μ₂ - μ₁) * (starRingEnd ℂ (vecToC (e₁ t)) * vecToC (e₂ t)).re) t := by
  sorry

end FiniteEnergyPlane
Source
C. Wendl, Lectures on Symplectic Field Theory (2026 notes), arXiv:1612.01009, Section 3.7, proof of Theorem 3.7.1; H. Hofer, K. Wysocki, E. Zehnder, GAFA 5 (1995), Section 3.

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