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Curves of zeros of the weighted operator give families of Jˉ\bar JJˉ-holomorphic planes

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FiniteEnergyPlane.exists_jbar_family_of_qMap_curve

by Mazecto · Nov 12, 2026 · Mathlib 0df444a (Lean v4.33.1)

elliptic-pdepseudoholomorphic-curvessymplectic-geometry

Let ρ,b>0\rho, b > 0ρ,b>0, let (Jˉ,J∞,S∞)(\bar J, J_\infty, S_\infty)(Jˉ,J∞​,S∞​) be a standard tube structure (IsStdTubeStructure ρ b Jbar Jinf Sinf), let δ<0\delta < 0δ<0 and δT∈(max⁡(δ,−2π),0)\delta_T \in (\max(\delta, -2\pi), 0)δT​∈(max(δ,−2π),0), let χT,χN,β\chi_T, \chi_N, \betaχT​,χN​,β satisfy IsSlopeWeight χT π (2π + δT), IsSlopeWeight χN π δ and IsLeftCutoff β, and let l∈Nl \in \mathbb{N}l∈N. Then there is ε0>0\varepsilon_0 > 0ε0​>0 with the following property.

Let r>0r > 0r>0 and let γ:R→W1,4×C×W1,4\gamma : \mathbb{R} \to W^{1,4} \times \mathbb{C} \times W^{1,4}γ:R→W1,4×C×W1,4 be C∞C^\inftyC∞ on (−r,r)(-r, r)(−r,r), with γ(0)=0\gamma(0) = 0γ(0)=0, γ′(0)=k\gamma'(0) = kγ′(0)=k, and, for every t∈(−r,r)t \in (-r, r)t∈(−r,r), γ(t)∈Bε0(0)\gamma(t) \in B_{\varepsilon_0}(0)γ(t)∈Bε0​​(0) and qMap Jbar χT χN β (γ t) = 0. Then there are r1>0r_1 > 0r1​>0 and G:C×R→C×CG : \mathbb{C} \times \mathbb{R} \to \mathbb{C} \times \mathbb{C}G:C×R→C×C, ClC^lCl on C×(−r1,r1)\mathbb{C} \times (-r_1, r_1)C×(−r1​,r1​), such that

  • G(z,0)=(z,0)G(z, 0) = (z, 0)G(z,0)=(z,0) for all zzz, and [∂tG(0,0)]2=k2\big[\partial_t G(0,0)\big]_2 = k_2[∂t​G(0,0)]2​=k2​, the C\mathbb{C}C-component of kkk;
  • for each t∈(−r1,r1)t \in (-r_1, r_1)t∈(−r1​,r1​) the map Gt=(ψt,vt)G_t = (\psi_t, v_t)Gt​=(ψt​,vt​) is C∞C^\inftyC∞, takes values in C×Bρ(0)\mathbb{C} \times B_\rho(0)C×Bρ​(0), is Jˉ\bar JJˉ-holomorphic on C\mathbb{C}C, and satisfies, for some CCC and β′>0\beta' > 0β′>0, ∣ψt(z)−z∣≤C(1+∣z∣)1−β′|\psi_t(z) - z| \le C(1+|z|)^{1-\beta'}∣ψt​(z)−z∣≤C(1+∣z∣)1−β′, ∣vt(z)∣≤C(1+∣z∣)δ/2π|v_t(z)| \le C(1+|z|)^{\delta/2\pi}∣vt​(z)∣≤C(1+∣z∣)δ/2π, and for every zzz there is Δ\DeltaΔ with [DG(z,t)(Δ,1)]1=0\big[DG(z,t)(\Delta,1)\big]_1 = 0[DG(z,t)(Δ,1)]1​=0 and ∣[DG(z,t)(Δ,1)]2∣≤C(1+∣z∣)δ/2π\big|\big[DG(z,t)(\Delta,1)\big]_2\big| \le C(1+|z|)^{\delta/2\pi}​[DG(z,t)(Δ,1)]2​​≤C(1+∣z∣)δ/2π;
  • for every ε>0\varepsilon > 0ε>0 there is r′∈(0,r1]r' \in (0, r_1]r′∈(0,r1​] such that for ∣t∣<r′|t| < r'∣t∣<r′ and all zzz: ∣ψt(z)−z∣≤ε(1+∣z∣)|\psi_t(z) - z| \le \varepsilon(1+|z|)∣ψt​(z)−z∣≤ε(1+∣z∣), ∣vt(z)∣≤ε|v_t(z)| \le \varepsilon∣vt​(z)∣≤ε, ∥Dψt(z)−id∥≤ε\|D\psi_t(z) - \mathrm{id}\| \le \varepsilon∥Dψt​(z)−id∥≤ε and (1+∣z∣)∥Dvt(z)∥≤ε(1+|z|)\|Dv_t(z)\| \le \varepsilon(1+∣z∣)∥Dvt​(z)∥≤ε.

The hypothesis that every member γ(t)\gamma(t)γ(t) is a zero is essential.

Role. Weak solutions of the Jˉ\bar JJˉ-Cauchy–Riemann equation in weighted Sobolev coordinates are turned into an honest family of smooth Jˉ\bar JJˉ-holomorphic planes, jointly regular in the parameter, with pointwise weighted bounds.

Preamble
import Definitions.Def_FiniteEnergyPlane_TubeFamily
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology CauchyRiemannIndex
open scoped ContDiff ENNReal Real

/-- For a standard tube structure there is `ε₀ > 0` such that every `C^∞` curve `γ` of zeros of
`qMap` in `ball 0 ε₀` (every member a zero) with `γ 0 = 0` and velocity `k` at `0` defines a jointly
`C^l` family `G(·, t)` of `Jbar`-holomorphic planes through `G(·, 0) = (z, 0)`, with normal
velocity `k.2.1` at `z = 0`, the weighted bounds on each member, and weighted `C¹` convergence to
`(z, 0)` as `t → 0`. -/
theorem exists_jbar_family_of_qMap_curve (ρ b : ℝ) (hρ : 0 < ρ) (hb : 0 < b)
    (Jbar : ℂ × ℂ → ℂ × ℂ →L[ℝ] ℂ × ℂ) (Jinf : ℝ × ℂ → ℂ × ℂ →L[ℝ] ℂ × ℂ)
    (Sinf : ℝ → Mat 1) (hstd : IsStdTubeStructure ρ b Jbar Jinf Sinf)
    (δ δT : ℝ) (hδ : δ < 0) (hδT : δT ∈ Set.Ioo (max δ (-(2 * π))) 0)
    (χT χN β : ℝ → ℝ) (hχT : IsSlopeWeight χT π (2 * π + δT)) (hχN : IsSlopeWeight χN π δ)
    (hβ : IsLeftCutoff β) (l : ℕ) :
    ∃ ε₀ > 0, ∀ r > 0, ∀ (γ : ℝ → QDom) (k : QDom), ContDiffOn ℝ ∞ γ (Set.Ioo (-r) r) →
      γ 0 = 0 → HasDerivAt γ k 0 →
      (∀ t ∈ Set.Ioo (-r) r, γ t ∈ ball 0 ε₀ ∧ qMap Jbar χT χN β (γ t) = 0) →
    ∃ r > 0, ∃ G : ℂ × ℝ → ℂ × ℂ, ContDiffOn ℝ l G (Set.univ ×ˢ Set.Ioo (-r) r) ∧
      (∀ z, G (z, 0) = (z, 0)) ∧ (fderiv ℝ G (0, 0) (0, 1)).2 = k.2.1 ∧
      (∀ t ∈ Set.Ioo (-r) r,
        ContDiff ℝ ∞ (fun z => G (z, t)) ∧ (∀ z, (G (z, t)).2 ∈ ball (0 : ℂ) ρ) ∧
        JHolomorphic.IsJHolomorphicOn Jbar Set.univ (fun z => G (z, t)) ∧
        (∃ C β : ℝ, 0 < β ∧ ∀ z, ‖(G (z, t)).1 - z‖ ≤ C * (1 + ‖z‖) ^ (1 - β)) ∧
        (∃ C : ℝ, ∀ z, ‖(G (z, t)).2‖ ≤ C * (1 + ‖z‖) ^ (δ / (2 * π))) ∧
        ∃ C : ℝ, ∀ z, ∃ Δ : ℂ, (fderiv ℝ G (z, t) (Δ, 1)).1 = 0 ∧
          ‖(fderiv ℝ G (z, t) (Δ, 1)).2‖ ≤ C * (1 + ‖z‖) ^ (δ / (2 * π))) ∧
      ∀ ε > 0, ∃ r' ∈ Set.Ioc 0 r, ∀ t ∈ Set.Ioo (-r') r', ∀ z,
        ‖(G (z, t)).1 - z‖ ≤ ε * (1 + ‖z‖) ∧ ‖(G (z, t)).2‖ ≤ ε ∧
        ‖fderiv ℝ (fun z => (G (z, t)).1) z - ContinuousLinearMap.id ℝ ℂ‖ ≤ ε ∧
        (1 + ‖z‖) * ‖fderiv ℝ (fun z => (G (z, t)).2) z‖ ≤ ε := by
  sorry

end FiniteEnergyPlane
Source
Toward U. Hryniewicz, Fast finite-energy planes in symplectizations and applications, Trans. AMS 364 (2012), arXiv:0812.4076, Lemmas 6.10 and 6.20 (families of fast planes); operators in the setting of C. Wendl, Lectures on Holomorphic Curves in Symplectic and Contact Geometry, arXiv:1011.1690, Ch. 4

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