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A finite-energy curve on a punctured disc, read on the punctured unit disc

Proved
FiniteEnergyPlane.isFiniteEnergyCurve_comp_affine

by Mazecto · Nov 3, 2026 · Mathlib 0df444a (Lean v4.33.1)

finite-energypseudoholomorphic-curvessymplectization

Let S=H−1(1)⊂R2n+2S=H^{-1}(1)\subset\mathbb{R}^{2n+2}S=H−1(1)⊂R2n+2, let JJJ be a complex structure on ξ\xiξ and J~\tilde JJ~ the induced almost complex structure on R2n+2∖{0}≅R×S\mathbb{R}^{2n+2}\setminus\{0\}\cong\mathbb{R}\times SR2n+2∖{0}≅R×S. Let z0∈Cz_0\in\mathbb{C}z0​∈C, r>0r>0r>0, and let uuu be a finite-energy J~\tilde JJ~-holomorphic curve on the punctured disc B(z0,r)∖{z0}B(z_0,r)\setminus\{z_0\}B(z0​,r)∖{z0​} (smooth, avoiding 000, J~\tilde JJ~-holomorphic, with finite Hofer energy). Then u~(z)=u(z0+rz)\tilde u(z)=u(z_0+rz)u~(z)=u(z0​+rz) is a finite-energy J~\tilde JJ~-holomorphic curve on the punctured unit disc B(0,1)∖{0}B(0,1)\setminus\{0\}B(0,1)∖{0}, and for every z∈Cz\in\mathbb{C}z∈C

D(pr∘u~)(z)=r D(pr∘u)(z0+rz).D(\mathrm{pr}\circ\tilde u)(z)=r\,D(\mathrm{pr}\circ u)(z_0+rz).D(pr∘u~)(z)=rD(pr∘u)(z0​+rz).

This moves statements about finite-energy curves near the puncture 000 of the unit disc to an arbitrary puncture z0z_0z0​ of a disc of any radius.

Formalization Note R2n+2\mathbb{R}^{2n+2}R2n+2 is V n, J~\tilde JJ~ is Jtilde H J, pr\mathrm{pr}pr is proj H; "finite-energy curve on UUU" is IsFiniteEnergyCurve H J U. No hypothesis on HHH or JJJ is needed.

Preamble
import Definitions.Def_FiniteEnergyPlane_Setting
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- A finite-energy `J̃`-holomorphic curve on the punctured disc `B(z₀, r) \ {z₀}`, read in the
coordinate `z ↦ z₀ + r z`, is a finite-energy `J̃`-holomorphic curve on the punctured unit disc,
and the derivative of its projection to `S` is `r` times that of `u` at `z₀ + r z`. -/
theorem isFiniteEnergyCurve_comp_affine {n : ℕ} (H : V n → ℝ) (J : V n → V n →L[ℝ] V n)
    (z₀ : ℂ) (r : ℝ) (hr : 0 < r) (u : ℂ → V n)
    (hu : IsFiniteEnergyCurve H J (ball z₀ r \ {z₀}) u) :
    IsFiniteEnergyCurve H J (ball 0 1 \ {0}) (fun z => u (z₀ + (r : ℂ) * z)) ∧
      ∀ z : ℂ, fderiv ℝ (fun z => proj H (u (z₀ + (r : ℂ) * z))) z =
        r • fderiv ℝ (fun z => proj H (u z)) (z₀ + (r : ℂ) * z) := by
  sorry

end FiniteEnergyPlane
Source
H. Hofer, K. Wysocki, E. Zehnder; U. Hryniewicz, J. Symplectic Geom. 12 (2014), arXiv:1105.2077, Section 2.2 (finite-energy curves near a puncture; standard change of coordinates)

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