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Fourier coefficients of a real L2L^2L2 loop are conjugate-symmetric

Proved
AsymptoticOperator.coeff_neg

by Mazecto · Oct 10, 2026 · Mathlib 0df444a (Lean v4.33.1)

asymptotic-operatorfourier-analysisspectral-theory

Let f∈L2(R/Z,R2n)f\in L^2(\mathbb{R}/\mathbb{Z},\mathbb{R}^{2n})f∈L2(R/Z,R2n) (with the Haar probability measure) and let f^k=∫R/Ze−2πiktf(t) dt∈C2n\hat f_k=\int_{\mathbb{R}/\mathbb{Z}} e^{-2\pi i k t} f(t)\,dt\in\mathbb{C}^{2n}f^​k​=∫R/Z​e−2πiktf(t)dt∈C2n be its Fourier coefficients, computed componentwise on the complexification. Then for every k∈Zk\in\mathbb{Z}k∈Z and every coordinate iii,

(f^−k)i=(f^k)i‾.(\hat f_{-k})_i=\overline{(\hat f_k)_i}.(f^​−k​)i​=(f^​k​)i​​.

Role: the reality condition on Fourier coefficients of real loops, used throughout the spectral theory of the asymptotic operators AS=−J0∂t−SA_S=-J_0\partial_t-SAS​=−J0​∂t​−S.

Formalization note: L2 n, coeff are from Definitions.Def_AsymptoticOperator_Setting; coordinates are indexed by Fin n ⊕ Fin n; complex conjugation is starRingEnd ℂ.

Preamble
import Definitions.Def_AsymptoticOperator_Setting
Formal statement
namespace AsymptoticOperator

open ConleyZehnder

/-- The Fourier coefficients of a real `L²` function on the circle are conjugate-symmetric:
`f̂₋ₖ = conj f̂ₖ` componentwise. -/
theorem coeff_neg {n : ℕ} (f : L2 n) (k : ℤ) (i : Fin n ⊕ Fin n) :
    coeff f (-k) i = (starRingEnd ℂ) (coeff f k i) := by sorry

end AsymptoticOperator
Source
Standard Fourier-analysis fact; used for Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, §3.4, p. 63

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