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Winding number of a JJJ-holomorphic curve in coordinates adapted to an immersed curve

Proved
FiniteEnergyPlane.exists_normal_chart_hasLoopWind

by Mazecto · Nov 5, 2026 · Mathlib 0df444a (Lean v4.33.1)

pseudoholomorphic-curvessymplectic-geometrywinding-number

Let EEE be a real vector space of dimension 444, O⊂EO\subset EO⊂E open, and JJJ a smooth almost complex structure on OOO. Let U,W⊂CU,W\subset\mathbb{C}U,W⊂C be open and let u:U→Ou:U\to Ou:U→O, v:W→Ov:W\to Ov:W→O be smooth JJJ-holomorphic maps, z0∈Uz_0\in Uz0​∈U, w0∈Ww_0\in Ww0​∈W, u(z0)=v(w0)u(z_0)=v(w_0)u(z0​)=v(w0​), with Dv(w0)Dv(w_0)Dv(w0​) injective, and suppose this intersection is isolated: for some ε>0\varepsilon>0ε>0, the only pair (z,w)∈Bε(z0)×Bε(w0)(z,w)\in B_\varepsilon(z_0)\times B_\varepsilon(w_0)(z,w)∈Bε​(z0​)×Bε​(w0​) with u(z)=v(w)u(z)=v(w)u(z)=v(w) is (z0,w0)(z_0,w_0)(z0​,w0​).

Then there are a map Ψ:C×C→E\Psi:\mathbb{C}\times\mathbb{C}\to EΨ:C×C→E with Ψ(ζ,0)=v(w0+ζ)\Psi(\zeta,0)=v(w_0+\zeta)Ψ(ζ,0)=v(w0​+ζ) for all ζ\zetaζ, which is C1C^1C1 at the origin with invertible derivative there, and a map Ξ:E→C×C\Xi:E\to\mathbb{C}\times\mathbb{C}Ξ:E→C×C, continuous at u(z0)u(z_0)u(z0​) with Ξ(u(z0))=0\Xi(u(z_0))=0Ξ(u(z0​))=0 and Ψ∘Ξ=id\Psi\circ\Xi=\mathrm{id}Ψ∘Ξ=id near u(z0)u(z_0)u(z0​), and an integer m≥1m\ge 1m≥1 and r>0r>0r>0, such that for all ρ∈(0,r)\rho\in(0,r)ρ∈(0,r) the loop t↦pr2 Ξ(u(z0+ρe2πit))t\mapsto \mathrm{pr}_2\,\Xi\big(u(z_0+\rho e^{2\pi i t})\big)t↦pr2​Ξ(u(z0​+ρe2πit)) lies in C∖{0}\mathbb{C}\setminus\{0\}C∖{0} with winding number mmm.

Role: measures the local intersection multiplicity of uuu with the immersed curve vvv by the winding number of a single complex-valued function in a coordinate system in which vvv is the first axis.

Formalization Note "Smooth almost complex structure" is JHolomorphic.IsAlmostComplexOn, and "JJJ-holomorphic" is JHolomorphic.IsJHolomorphicOn. The maps are functions on all of C\mathbb{C}C and EEE, constrained only on the indicated sets; the isolation condition concerns the values of uuu and vvv on the two discs, which need not lie in UUU and WWW.

Preamble
import Definitions.Def_FiniteEnergyPlane_Winding
Formal statement
namespace FiniteEnergyPlane

open Metric Filter Topology
open scoped ContDiff

/-- Let `J` be a smooth almost complex structure on an open subset `O` of a real `4`-dimensional space
`E`, and let `u`, `v` be smooth `J`-holomorphic maps from open subsets of `ℂ` to `O` with
`u(z₀) = v(w₀)` an isolated intersection and `Dv(w₀)` injective. Then there are a map
`Ψ : ℂ × ℂ → E` with `Ψ(ζ, 0) = v(w₀ + ζ)`, `C¹` at `0` with invertible derivative there, and a local
right inverse `Ξ` of `Ψ` near `u(z₀)`, continuous at `u(z₀)` with `Ξ(u(z₀)) = 0`, such that the second
component of `Ξ ∘ u` has a winding number `m ≥ 1` along all small counterclockwise circles about
`z₀`. -/
theorem exists_normal_chart_hasLoopWind {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E]
    [FiniteDimensional ℝ E] (hE : Module.finrank ℝ E = 4) (J : E → E →L[ℝ] E) (O : Set E)
    (hJ : JHolomorphic.IsAlmostComplexOn J O) (U W : Set ℂ) (hU : IsOpen U) (hW : IsOpen W)
    (u v : ℂ → E) (hu : ContDiffOn ℝ ∞ u U) (hv : ContDiffOn ℝ ∞ v W)
    (huO : Set.MapsTo u U O) (hvO : Set.MapsTo v W O)
    (huh : JHolomorphic.IsJHolomorphicOn J U u) (hvh : JHolomorphic.IsJHolomorphicOn J W v)
    (z₀ w₀ : ℂ) (hz₀ : z₀ ∈ U) (hw₀ : w₀ ∈ W) (h₀ : u z₀ = v w₀)
    (hvi : Function.Injective (fderiv ℝ v w₀))
    (hiso : ∃ ε > 0, ∀ z ∈ ball z₀ ε, ∀ w ∈ ball w₀ ε, u z = v w → z = z₀ ∧ w = w₀) :
    ∃ (Ψ : ℂ × ℂ → E) (Ξ : E → ℂ × ℂ) (e : (ℂ × ℂ) ≃L[ℝ] E),
      ContDiffAt ℝ 1 Ψ (0, 0) ∧ fderiv ℝ Ψ (0, 0) = (e : ℂ × ℂ →L[ℝ] E) ∧
      (∀ ζ, Ψ (ζ, 0) = v (w₀ + ζ)) ∧ ContinuousAt Ξ (u z₀) ∧ Ξ (u z₀) = (0, 0) ∧
      (∀ᶠ x in 𝓝 (u z₀), Ψ (Ξ x) = x) ∧
      ∃ m : ℕ, 1 ≤ m ∧ ∃ r > (0 : ℝ), ∀ ρ ∈ Set.Ioo 0 r,
        HasLoopWind (fun t => (Ξ (u (z₀ + ccwLoop ρ t))).2) m := by
  sorry

end FiniteEnergyPlane
Source
Cf. D. McDuff, J. Differential Geom. 34 (1991), 143-164, Section 5; M. Micallef, B. White, Ann. of Math. 141 (1995)

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