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Limit at a finite-energy puncture of a pseudoholomorphic map

Proved
FiniteEnergyPlane.exists_tendsto_of_energy_lt_top

by Mazecto · Oct 24, 2026 · Mathlib 0df444a (Lean v4.33.1)

elliptic-regularityfinite-energypseudoholomorphic-curvessymplectic-geometry

Let EEE be a finite-dimensional real normed space, JJJ a smooth almost complex structure on an open set O⊆EO\subseteq EO⊆E, and K⊆OK\subseteq OK⊆O compact. Let D⊂CD\subset\mathbb{C}D⊂C be the open unit disc and uuu a C∞C^\inftyC∞ JJJ-holomorphic map on D∖{0}D\setminus\{0\}D∖{0} with u(D∖{0})⊆Ku(D\setminus\{0\})\subseteq Ku(D∖{0})⊆K,

∫D∖{0}∥Du(z)∥2 dz<∞,\int_{D\setminus\{0\}}\|Du(z)\|^2\,dz<\infty,∫D∖{0}​∥Du(z)∥2dz<∞,

and assume there are r>0r>0r>0 and CCC with ∣z∣ ∥Du(z)∥≤C|z|\,\|Du(z)\|\le C∣z∣∥Du(z)∥≤C for 0<∣z∣<r0<|z|<r0<∣z∣<r. Then u(z)u(z)u(z) converges as z→0z\to 0z→0: there is x0∈Ex_0\in Ex0​∈E with u(z)→x0u(z)\to x_0u(z)→x0​ as z→0z\to0z→0, z≠0z\ne0z=0.

This is the continuity part of the removable singularity theorem: a finite-energy puncture with the stated gradient bound has a continuous extension.

Formalization Note The energy is a lower integral in ℝ≥0∞ of the squared operator norm of fderiv ℝ u. The limit is Tendsto u (𝓝[≠] 0) (𝓝 x₀).

Preamble
import Definitions.Def_FiniteEnergyPlane_Setting
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Limit at a puncture (Wendl, Theorem 9.2, continuity part, (9.1)). Let `J` be a smooth almost
complex structure on an open set `O ⊆ E` and `K ⊆ O` compact. A smooth `J`-holomorphic map on the
punctured unit disc with values in `K`, finite Dirichlet energy `∫ ‖Du‖²` and `|z| ‖Du(z)‖` bounded
near the puncture has a limit at the puncture. -/
theorem exists_tendsto_of_energy_lt_top {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] (J : E → E →L[ℝ] E) (O : Set E)
    (hJ : JHolomorphic.IsAlmostComplexOn J O) (K : Set E) (hK : IsCompact K) (hKO : K ⊆ O)
    (u : ℂ → E) (hu : ContDiffOn ℝ ∞ u (ball 0 1 \ {0}))
    (hhol : JHolomorphic.IsJHolomorphicOn J (ball 0 1 \ {0}) u)
    (hmaps : Set.MapsTo u (ball 0 1 \ {0}) K)
    (hE : ∫⁻ z in ball 0 1 \ {0}, ENNReal.ofReal (‖fderiv ℝ u z‖ ^ 2) < ⊤)
    (hG : ∃ r : ℝ, 0 < r ∧ ∃ C : ℝ, ∀ z : ℂ, z ≠ 0 → ‖z‖ < r → ‖z‖ * ‖fderiv ℝ u z‖ ≤ C) :
    ∃ x₀ : E, Tendsto u (𝓝[≠] 0) (𝓝 x₀) := by
  sorry

end FiniteEnergyPlane
Source
C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, Theorem 9.2 and (9.1), pp. 152-155

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