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Gradient bound near a finite-energy puncture of a pseudoholomorphic map

Proved
FiniteEnergyPlane.exists_norm_mul_fderiv_le_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 and

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

Then there are r>0r>0r>0 and CCC such that

∣z∣ ∥Du(z)∥≤Cfor all 0<∣z∣<r.|z|\,\|Du(z)\|\le C\qquad\text{for all } 0<|z|<r .∣z∣∥Du(z)∥≤Cfor all 0<∣z∣<r.

In cylindrical coordinates z=e−2π(s+it)z=e^{-2\pi(s+it)}z=e−2π(s+it) this says that the derivative of uuu is bounded on a half-cylinder end. It is the gradient bound used to show that a finite-energy puncture is removable.

Formalization Note The energy is a lower integral in ℝ≥0∞ of the squared operator norm of fderiv ℝ u. The conclusion is ∃ r > 0, ∃ C, ∀ z ≠ 0, ‖z‖ < r → ‖z‖ * ‖fderiv ℝ u z‖ ≤ C.

Preamble
import Definitions.Def_FiniteEnergyPlane_Setting
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Gradient bound at a puncture (Wendl, Lemma 9.3, in disc coordinates). 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` and finite Dirichlet energy `∫ ‖Du‖²` satisfies
`|z| ‖Du(z)‖ ≤ C` for all `z ≠ 0` in some disc about the puncture. -/
theorem exists_norm_mul_fderiv_le_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) < ⊤) :
    ∃ r : ℝ, 0 < r ∧ ∃ C : ℝ, ∀ z : ℂ, z ≠ 0 → ‖z‖ < r → ‖z‖ * ‖fderiv ℝ u z‖ ≤ C := by
  sorry

end FiniteEnergyPlane
Source
C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, Lemma 9.3, p. 153

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