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A loop missing a ray from the origin has winding number zero

Proved
FiniteEnergyPlane.hasLoopWind_zero_of_forall_ne_ray

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

complex-analysissymplectic-geometrytopologywinding-numbers

Let q:R→Cq:\mathbb{R}\to\mathbb{C}q:R→C be continuous and 111-periodic, and let w∈C∖{0}w\in\mathbb{C}\setminus\{0\}w∈C∖{0}. If q(t)≠s wq(t)\neq s\,wq(t)=sw for every t∈Rt\in\mathbb{R}t∈R and every real s≥0s\ge 0s≥0 (so qqq avoids the closed ray from 000 through www, including 000), then qqq has winding number 000.

A criterion for vanishing winding, for comparing windings of loops in C∖{0}\mathbb{C}\setminus\{0\}C∖{0}.

Formalization Note The conclusion is HasLoopWind q 0 from FiniteEnergyPlane_Winding; the hypothesis is ∀ t, ∀ s : ℝ, 0 ≤ s → q t ≠ s * w with hw : w ≠ 0.

Preamble
import Definitions.Def_FiniteEnergyPlane_Winding
Formal statement
namespace FiniteEnergyPlane

/-- A continuous `1`-periodic loop in `ℂ` that misses a closed ray `{s w : s ≥ 0}` (`w ≠ 0`)
has winding number `0`. -/
theorem hasLoopWind_zero_of_forall_ne_ray (q : ℝ → ℂ) (hq : Continuous q)
    (hper : Function.Periodic q 1) (w : ℂ) (hw : w ≠ 0)
    (h : ∀ t, ∀ s : ℝ, 0 ≤ s → q t ≠ s * w) : HasLoopWind q 0 := 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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