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Continuous periodic loops in C∖{0}\mathbb{C}\setminus\{0\}C∖{0} have a winding number

Proved
FiniteEnergyPlane.exists_hasLoopWind

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

complex-analysissymplectic-geometrytopologywinding-numbers

Let f:R→Cf:\mathbb{R}\to\mathbb{C}f:R→C be continuous, 111-periodic and nowhere zero. Then fff has an integer winding number kkk: there is a continuous θ:R→R\theta:\mathbb{R}\to\mathbb{R}θ:R→R with f(t)=∣f(t)∣eiθ(t)f(t)=|f(t)|e^{i\theta(t)}f(t)=∣f(t)∣eiθ(t) for all t∈Rt\in\mathbb{R}t∈R and θ(1)−θ(0)=2πk\theta(1)-\theta(0)=2\pi kθ(1)−θ(0)=2πk.

This is the basic existence statement for the winding invariant HasLoopWind used throughout the winding-number milestones of finite-energy planes.

Formalization Note The conclusion is ∃ k : ℤ, HasLoopWind f k with HasLoopWind from FiniteEnergyPlane_Winding; the angle function θ\thetaθ is required on all of R\mathbb{R}R, not only on [0,1][0,1][0,1].

Preamble
import Definitions.Def_FiniteEnergyPlane_Winding
Formal statement
namespace FiniteEnergyPlane

/-- A continuous `1`-periodic loop in `ℂ \ {0}` has a winding number. -/
theorem exists_hasLoopWind (f : ℝ → ℂ) (hf : Continuous f) (hper : Function.Periodic f 1)
    (h0 : ∀ t, f t ≠ 0) : ∃ k : ℤ, HasLoopWind f k := by
  sorry

end FiniteEnergyPlane
Source
C. Wendl, Lectures on Symplectic Field Theory (2026 notes), arXiv:1612.01009, Section 3.7 (winding numbers of loops in C minus 0); standard.

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