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Solutions of real-linear Cauchy–Riemann equations factor locally through holomorphic maps

Proved
JHolomorphic.exists_holomorphic_factorization

by Mazecto · Oct 20, 2026 · Mathlib 0df444a (Lean v4.33.1)

elliptic-regularitypseudoholomorphic-curvessobolev-spacessymplectic-geometryunique-continuation

Let EEE be a real vector space of dimension 2n2n2n, let D⊂CD\subset\mathbb{C}D⊂C be the open unit disc, and let Jˉ,A:D→End⁡R(E)\bar J,A:D\to\operatorname{End}_{\mathbb{R}}(E)Jˉ,A:D→EndR​(E) be C∞C^\inftyC∞ with Jˉ(z)2=−Id\bar J(z)^2=-\mathrm{Id}Jˉ(z)2=−Id. Let h:D→Eh:D\to Eh:D→E be C∞C^\inftyC∞ with

∂sh+Jˉ(z) ∂th+A(z) h=0on D.\partial_sh+\bar J(z)\,\partial_th+A(z)\,h=0\quad\text{on }D.∂s​h+Jˉ(z)∂t​h+A(z)h=0on D.

Then there are ε>0\varepsilon>0ε>0, a continuous map Φ\PhiΦ from the closed disc Dˉε\bar D_\varepsilonDˉε​ to the real-linear maps Cn→E\mathbb{C}^n\to ECn→E, each Φ(z)\Phi(z)Φ(z) bijective with Φ(z)(iw)=Jˉ(z) Φ(z)w\Phi(z)(iw)=\bar J(z)\,\Phi(z)wΦ(z)(iw)=Jˉ(z)Φ(z)w, and a holomorphic f:Dε→Cnf:D_\varepsilon\to\mathbb{C}^nf:Dε​→Cn, such that

h(z)=Φ(z) f(z)for z∈Dε.h(z)=\Phi(z)\,f(z)\quad\text{for }z\in D_\varepsilon.h(z)=Φ(z)f(z)for z∈Dε​.

Formalization Note Wendl's Theorem 2.26 is the case E=CnE=\mathbb{C}^nE=Cn, Jˉ≡i\bar J\equiv iJˉ≡i, and assumes in addition h(0)=0h(0)=0h(0)=0. EEE is a normed space with Module.finrank ℝ E = 2 * n, Cn\mathbb{C}^nCn is EuclideanSpace ℂ (Fin n), Φ\PhiΦ has type ℂ → EuclideanSpace ℂ (Fin n) →L[ℝ] E with ContinuousOn Φ (closedBall 0 ε), and fff satisfies DifferentiableOn ℂ f (ball 0 ε).

Preamble
import Definitions.Def_JHolomorphic_Setting
Formal statement
namespace JHolomorphic

open MeasureTheory Metric Filter Topology DbarRegularity
open scoped ContDiff ENNReal NNReal

/-- Wendl, Theorem 2.26 (p. 39), generalized to a complex structure that varies with the
point: let `E` have real dimension `2n`, let `J̄ : D → End_ℝ(E)` be smooth on the open
unit disc `D` with `J̄(z)² = -1`, let `A : D → End_ℝ(E)` be smooth, and let `h : D → E` be smooth
with `∂ₛh + J̄(z) ∂ₜh + A(z) h = 0`. For some `ε > 0` there are a continuous
`Φ : D̄_ε → Hom_ℝ(ℂⁿ, E)` with every `Φ(z)` bijective and `Φ(z) ∘ i = J̄(z) ∘ Φ(z)`, and a
holomorphic `f : D_ε → ℂⁿ` with `h = Φ f` on `D_ε`. (Wendl's Theorem 2.26 is the case
`E = ℂⁿ`, `J̄ ≡ i`; he also assumes `h(0) = 0`.) -/
theorem exists_holomorphic_factorization {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] (n : ℕ)
    (hn : Module.finrank ℝ E = 2 * n) (Jbar A : ℂ → E →L[ℝ] E)
    (hJbar : ContDiffOn ℝ ∞ Jbar (ball 0 1))
    (hJbar2 : ∀ z ∈ ball (0 : ℂ) 1, (Jbar z).comp (Jbar z) = -ContinuousLinearMap.id ℝ E)
    (hA : ContDiffOn ℝ ∞ A (ball 0 1)) (h : ℂ → E) (hh : ContDiffOn ℝ ∞ h (ball 0 1))
    (heq : ∀ z ∈ ball (0 : ℂ) 1,
      fderiv ℝ h z 1 + Jbar z (fderiv ℝ h z Complex.I) + A z (h z) = 0) :
    ∃ ε > (0 : ℝ), ∃ Φ : ℂ → EuclideanSpace ℂ (Fin n) →L[ℝ] E,
      ∃ f : ℂ → EuclideanSpace ℂ (Fin n), ContinuousOn Φ (closedBall 0 ε) ∧
        (∀ z ∈ closedBall (0 : ℂ) ε, Function.Bijective (Φ z) ∧
          ∀ w, Φ z (Complex.I • w) = Jbar z (Φ z w)) ∧
        DifferentiableOn ℂ f (ball 0 ε) ∧ ∀ z ∈ ball (0 : ℂ) ε, h z = Φ z (f z) := by
  sorry

end JHolomorphic
Source
C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, https://arxiv.org/abs/1612.01009, Lecture 2, Theorem 2.26, p. 39, generalized to a complex structure that varies with the point
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What the Lean code literally says, in plain math · claude-opus-5-5

JHolomorphic.exists_holomorphic_factorization

Setting. Let EEE be a finite-dimensional real normed vector space, and let n∈Nn \in \mathbb{N}n∈N be a natural number with dim⁡RE=2n\dim_{\mathbb{R}} E = 2ndimR​E=2n. (The case n=0n = 0n=0 is allowed; then E={0}E = \{0\}E={0}.) Write D={z∈C:∣z∣<1}\mathbb{D} = \{ z \in \mathbb{C} : |z| < 1 \}D={z∈C:∣z∣<1} for the open unit disc, and identify C\mathbb{C}C with R2\mathbb{R}^2R2 via z=s+itz = s + itz=s+it. The statement does not use any of the named definitions of the imported bundles (such as ∂ˉJ\bar\partial_J∂ˉJ​, JJJ-holomorphy, or weak JJJ-holomorphy); every condition below is written out directly.

Data and hypotheses. Given:

  • a map Jˉ:C→LR(E,E)\bar J : \mathbb{C} \to \mathcal{L}_{\mathbb{R}}(E, E)Jˉ:C→LR​(E,E) (continuous R\mathbb{R}R-linear endomorphisms of EEE, depending on the point z∈Cz \in \mathbb{C}z∈C, not on a point of EEE) which is C∞C^\inftyC∞ (smooth, in the real sense) on D\mathbb{D}D, and which satisfies
Jˉ(z)∘Jˉ(z)=−idEfor every z∈D;\bar J(z) \circ \bar J(z) = -\mathrm{id}_E \qquad \text{for every } z \in \mathbb{D};Jˉ(z)∘Jˉ(z)=−idE​for every z∈D;
  • a map A:C→LR(E,E)A : \mathbb{C} \to \mathcal{L}_{\mathbb{R}}(E, E)A:C→LR​(E,E) which is C∞C^\inftyC∞ on D\mathbb{D}D (no further condition on AAA);
  • a map h:C→Eh : \mathbb{C} \to Eh:C→E which is C∞C^\inftyC∞ on D\mathbb{D}D and satisfies, for every z∈Dz \in \mathbb{D}z∈D,
∂sh(z)+Jˉ(z) ∂th(z)+A(z) h(z)=0,\partial_s h(z) + \bar J(z)\,\partial_t h(z) + A(z)\,h(z) = 0,∂s​h(z)+Jˉ(z)∂t​h(z)+A(z)h(z)=0,

where ∂sh(z)=Dh(z)[1]\partial_s h(z) = Dh(z)[1]∂s​h(z)=Dh(z)[1] and ∂th(z)=Dh(z)[i]\partial_t h(z) = Dh(z)[i]∂t​h(z)=Dh(z)[i] are the values of the real Fréchet derivative of hhh at zzz on the vectors 111 and iii.

The values of Jˉ\bar JJˉ, AAA and hhh outside D\mathbb{D}D are unconstrained.

Conclusion. There exist a real number ε>0\varepsilon > 0ε>0, a map Φ:C→LR(Cn,E)\Phi : \mathbb{C} \to \mathcal{L}_{\mathbb{R}}(\mathbb{C}^n, E)Φ:C→LR​(Cn,E) (continuous R\mathbb{R}R-linear maps from Cn\mathbb{C}^nCn, with its Euclidean structure, to EEE), and a map f:C→Cnf : \mathbb{C} \to \mathbb{C}^nf:C→Cn such that:

  1. Φ\PhiΦ is continuous on the closed disc B‾(0,ε)={∣z∣≤ε}\overline{B}(0,\varepsilon) = \{ |z| \le \varepsilon \}B(0,ε)={∣z∣≤ε} (with respect to the operator-norm topology on LR(Cn,E)\mathcal{L}_{\mathbb{R}}(\mathbb{C}^n, E)LR​(Cn,E));
  2. for every zzz with ∣z∣≤ε|z| \le \varepsilon∣z∣≤ε, the R\mathbb{R}R-linear map Φ(z):Cn→E\Phi(z) : \mathbb{C}^n \to EΦ(z):Cn→E is bijective, and
Φ(z)(i w)=Jˉ(z)(Φ(z) w)for all w∈Cn;\Phi(z)(i\,w) = \bar J(z)\big(\Phi(z)\,w\big) \qquad \text{for all } w \in \mathbb{C}^n;Φ(z)(iw)=Jˉ(z)(Φ(z)w)for all w∈Cn;
  1. fff is complex-differentiable (holomorphic) at every point of the open disc B(0,ε)={∣z∣<ε}B(0,\varepsilon) = \{ |z| < \varepsilon \}B(0,ε)={∣z∣<ε};
  2. for every zzz with ∣z∣<ε|z| < \varepsilon∣z∣<ε,
h(z)=Φ(z)(f(z)).h(z) = \Phi(z)\big(f(z)\big).h(z)=Φ(z)(f(z)).

Remarks on what is and is not asserted. No upper bound on ε\varepsilonε is required; in particular ε≥1\varepsilon \ge 1ε≥1 is not excluded, in which case conditions 2 and 4 would also refer to points outside D\mathbb{D}D, where Jˉ\bar JJˉ and hhh are arbitrary (condition 2 forces Jˉ(z)2=−idE\bar J(z)^2 = -\mathrm{id}_EJˉ(z)2=−idE​ at every point of the closed disc). No regularity of Φ\PhiΦ beyond continuity on the closed disc is asserted, and nothing is asserted about fff or Φ\PhiΦ outside the respective discs. Nothing is asserted about fff being nonzero, and h≡0h \equiv 0h≡0 is allowed (then f≡0f \equiv 0f≡0 is permitted). The intertwining relation in condition 2 says that Φ(z)\Phi(z)Φ(z) carries multiplication by iii on Cn\mathbb{C}^nCn to Jˉ(z)\bar J(z)Jˉ(z) on EEE. When n=0n = 0n=0 all spaces involved are zero and every condition holds trivially for any ε>0\varepsilon > 0ε>0.

Human review
  • Endorsed by Shuze Chen · Oct 21, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Mazecto · Oct 21, 2026

    Confirmed by the mission captain (proposal self-audit).

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