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Transversality of a J-holomorphic family at one point holds along a fast member

Proved
FiniteEnergyPlane.fderiv_family_add_smul_eq_zero

by Mazecto · Nov 6, 2026 · Mathlib 0df444a (Lean v4.33.1)

pseudoholomorphic-curvessymplectic-geometry

Let S=H−1(1)⊂R4S = H^{-1}(1) \subset \mathbb{R}^4S=H−1(1)⊂R4 be a strictly star-shaped level with a compatible complex structure JJJ on the contact planes, and let PPP be a periodic Reeb orbit. Let δ<0\delta < 0δ<0 be such that every eigenvalue of the asymptotic operator APA_PAP​ below δ\deltaδ has winding number at most 111 and every eigenvalue above δ\deltaδ has winding number at least 222, in the global frame of ξ\xiξ. Let g:C×(−r,r)→V1g : \mathbb{C} \times (-r, r) \to V_1g:C×(−r,r)→V1​ be C2C^2C2 with every g(⋅,t′)g(\cdot, t')g(⋅,t′) J~\tilde JJ~-holomorphic, and let t∈(−r,r)t \in (-r, r)t∈(−r,r) be such that g(⋅,t)g(\cdot, t)g(⋅,t) is a fast finite-energy plane asymptotic to PPP at ∞\infty∞, ∂tg(⋅,t)\partial_t g(\cdot, t)∂t​g(⋅,t) is smooth, and for some CCC and every zzz some Δ∈C\Delta \in \mathbb{C}Δ∈C has ∣Dg(z,t)(Δ,1)∣≤C(1+∣z∣)δ/2π∣g(z,t)∣|Dg(z, t)(\Delta, 1)| \le C (1 + |z|)^{\delta/2\pi} |g(z, t)|∣Dg(z,t)(Δ,1)∣≤C(1+∣z∣)δ/2π∣g(z,t)∣.

If the identity Dg(0,t)(Δ,δt)+λ g(0,t)=0Dg(0, t)(\Delta, \delta t) + \lambda\, g(0, t) = 0Dg(0,t)(Δ,δt)+λg(0,t)=0 forces Δ=0\Delta = 0Δ=0, δt=0\delta t = 0δt=0 and λ=0\lambda = 0λ=0, then for every z∈Cz \in \mathbb{C}z∈C the identity Dg(z,t)(Δ,δt)+λ g(z,t)=0Dg(z, t)(\Delta, \delta t) + \lambda\, g(z, t) = 0Dg(z,t)(Δ,δt)+λg(z,t)=0 forces the same.

Role. The tangent plane of the member, the parameter direction and the R\mathbb{R}R-translation direction then span TV1T V_1TV1​ at every point of the member, not only at z=0z = 0z=0.

Formalization Note. The symplectization R×S\mathbb{R} \times SR×S is V1∖{0}V_1 \setminus \{0\}V1​∖{0}, with y=e2axy = e^{2a} xy=e2ax, aaa = aCoord H y and xxx = proj H y. Winding numbers are HasEigenWind; (1+∣z∣)δ/2π(1 + |z|)^{\delta/2\pi}(1+∣z∣)δ/2π is the cylindrical weight eδse^{\delta s}eδs for ∣z∣=e2πs|z| = e^{2\pi s}∣z∣=e2πs. The bound measures the ttt-derivative modulo the tangent plane of the member, relative to ∣g∣|g|∣g∣. The point z=0z = 0z=0 is only a convenient base point.

Preamble
import Definitions.Def_FiniteEnergyPlane_CylClose
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Transversality of a family of `J̃`-holomorphic maps at one point of a fast member holds along the
whole member. Let `δ < 0` be such that every eigenvalue of `A_P` below `δ` has winding number at most
`1` and every eigenvalue above `δ` has winding number at least `2`. Let `g : ℂ × (-r, r) → V 1` be
`C²` with every `g(·, t')` `J̃`-holomorphic, and let `g(·, t)` be a fast finite-energy plane
asymptotic to `P` at `∞`, with `∂ₜg(·, t)` smooth and with `Δ` at each `z` such that
`‖Dg(z, t)(Δ, 1)‖ ≤ C (1 + ‖z‖)^{δ/2π} ‖g(z, t)‖`. If `Dg(0, t)(Δ, δt) + λ • g(0, t) = 0` forces
`Δ = 0`, `δt = 0`, `λ = 0`, then the same holds with `0` replaced by any `z`. -/
theorem fderiv_family_add_smul_eq_zero (H : V 1 → ℝ) (hH : IsStrictlyStarShapedLevel H)
    (J : V 1 → V 1 →L[ℝ] V 1) (hJ : IsCompatibleXiStructure H J)
    (P : ReebOrbit H) (δ : ℝ) (hδ : δ < 0)
    (hwin : ∀ (μ : ℝ) (k : ℤ), HasEigenWind J P μ k → (μ < δ ∧ k ≤ 1) ∨ (δ < μ ∧ 2 ≤ k))
    (r : ℝ) (g : ℂ × ℝ → V 1) (hg : ContDiffOn ℝ 2 g (Set.univ ×ˢ Set.Ioo (-r) r))
    (hgJ : ∀ t' ∈ Set.Ioo (-r) r,
      JHolomorphic.IsJHolomorphicOn (Jtilde H J) Set.univ (fun z => g (z, t')))
    (t : ℝ) (ht : t ∈ Set.Ioo (-r) r)
    (hfast : IsFastPlane H J (fun z => g (z, t)))
    (hend : IsNondegenerateEnd H (fun z => g (z, t)) cylInf P 1)
    (hX : ContDiff ℝ ∞ (fun z => fderiv ℝ g (z, t) (0, 1)))
    (C : ℝ) (hrate : ∀ z, ∃ Δ : ℂ, ‖fderiv ℝ g (z, t) (Δ, 1)‖ ≤
      C * (1 + ‖z‖) ^ (δ / (2 * π)) * ‖g (z, t)‖)
    (htr : ∀ (Δ : ℂ) (δt lam : ℝ), fderiv ℝ g (0, t) (Δ, δt) + lam • g (0, t) = 0 →
      Δ = 0 ∧ δt = 0 ∧ lam = 0) (z : ℂ) (Δ : ℂ) (δt lam : ℝ)
    (h0 : fderiv ℝ g (z, t) (Δ, δt) + lam • g (z, t) = 0) :
    Δ = 0 ∧ δt = 0 ∧ lam = 0 := by
  sorry

end FiniteEnergyPlane
Source
U. Hryniewicz, Fast finite-energy planes in symplectizations and applications, Trans. AMS 364 (2012), arXiv:0812.4076, Lemma 6.10 and Lemma 6.20

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