Derivative of the cross term of two eigenfunctions of the asymptotic operator
ProvedFiniteEnergyPlane.hasDerivAt_im_conj_mul_loopEigenconley-zehnder-indexpseudoholomorphic-curvessymplectic-geometrywinding-numbers
Let be a continuous -periodic loop of symmetric matrices and on -periodic loops in . Let be eigenfunctions of with eigenvalues , viewed as loops in . Then for every ,
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, -periodic, not identically zero, ); symmetry and continuity are CauchyRiemannIndex.IsSymLoop Sinf; 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.