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Linear Cauchy–Riemann equation with exponentially convergent coefficients for the normal part of an end

Proved
FiniteEnergyPlane.exists_crEquation_tubeNormal_expDecay

by Mazecto · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

asymptotic-analysisasymptotic-operatorpseudoholomorphic-curvessymplectization

Let uuu be a finite-energy J~\tilde JJ~-holomorphic curve on D∖{0}D\setminus\{0\}D∖{0}, P=(x,T)P=(x,T)P=(x,T) a periodic Reeb orbit, ZZZ a unitary frame of ξ\xiξ along PPP in which the asymptotic operator is AP(Zη)=Z(−J0η′−S∞η)A_P(Z\eta)=Z(-J_0\eta'-S_\infty\eta)AP​(Zη)=Z(−J0​η′−S∞​η) with S∞S_\inftyS∞​ a smooth symmetric loop, ε=±1\varepsilon=\pm1ε=±1, and suppose the end w(s,t)w(s,t)w(s,t) of uuu at 000 is written for s≥s0s\ge s_0s≥s0​ as w=proj(x(τ)+h)w=\mathrm{proj}(x(\tau)+h)w=proj(x(τ)+h), h∈ξx(τ)h\in\xi_{x(\tau)}h∈ξx(τ)​, τ(s,t+1)=τ(s,t)+εT\tau(s,t+1)=\tau(s,t)+\varepsilon Tτ(s,t+1)=τ(s,t)+εT, hhh 111-periodic, with τ−εTt−c→0\tau-\varepsilon Tt-c\to0τ−εTt−c→0 and h→0h\to0h→0 in C∞C^\inftyC∞, and with

∣τ(s,t)−εTt−c∣+∥h(s,t)∥≤C0e−bs,b>0.|\tau(s,t)-\varepsilon Tt-c|+\|h(s,t)\|\le C_0e^{-bs},\qquad b>0.∣τ(s,t)−εTt−c∣+∥h(s,t)∥≤C0​e−bs,b>0.

Then there are s1s_1s1​, d>0d>0d>0, CCC and maps SSS (matrix valued) and ζ\zetaζ, smooth on (s1,∞)×R(s_1,\infty)\times\mathbb{R}(s1​,∞)×R, such that S(s,t)−εS∞(εt+c/T)S(s,t)-\varepsilon S_\infty(\varepsilon t+c/T)S(s,t)−εS∞​(εt+c/T) decays like e−dse^{-ds}e−ds in C∞C^\inftyC∞, and for s>s1s>s_1s>s1​: SSS, ζ\zetaζ are 111-periodic in ttt, ∂sζ+J0∂tζ+Sζ=0\partial_s\zeta+J_0\partial_t\zeta+S\zeta=0∂s​ζ+J0​∂t​ζ+Sζ=0, h=Z(τ/T)ζh=Z(\tau/T)\zetah=Z(τ/T)ζ and ∥ζ(s,t)∥≤Ce−ds\|\zeta(s,t)\|\le Ce^{-ds}∥ζ(s,t)∥≤Ce−ds.

This turns the normal part of an exponentially convergent end into a solution of a linear Cauchy–Riemann equation whose coefficients converge exponentially.

Formalization Note Exponential C∞C^\inftyC∞ convergence is IsExpAsymptoticTo (entrywise ExpDecayCInfty); the operator is CauchyRiemannIndex.crOp; the hypothesis on ZZZ, S∞S_\inftyS∞​ is the identity hZS for every smooth 111-periodic η\etaη.

Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Linear Cauchy–Riemann equation for the normal component of an end in tube coordinates, with
exponentially convergent coefficients. Let `u` be a finite-energy curve on `D \ {0}`, `P` a Reeb
orbit, `Z` a unitary frame of `ξ` along `P` in which `A_P` is `-J₀ ∂ₜ - S∞`, and suppose the end
is written as `w = proj H (x(τ) + h)`, `h ∈ ξ_{x(τ)}`, with `τ - εTt - c → 0` and `h → 0` in `C^∞`
and with `|τ - εTt - c| + ‖h‖ ≤ C₀ e^{-bs}`, `b > 0`. Then for some `s₁` and `d > 0` there are
`S` and `ζ`, smooth and `1`-periodic on `s > s₁`, with `h = Z(τ/T) ζ`, `∂ₛζ + J₀ ∂ₜζ + S ζ = 0`,
`‖ζ(s, t)‖ ≤ C e^{-ds}` for all `s > s₁`, and `S(s, t) - ε S∞(εt + c/T)` decaying like `e^{-ds}`
in `C^∞`. -/
theorem exists_crEquation_tubeNormal_expDecay {n : ℕ} (H : V n → ℝ)
    (hH : IsStrictlyStarShapedLevel H)
    (J : V n → V n →L[ℝ] V n) (hJ : IsCompatibleXiStructure H J) (u : ℂ → V n)
    (hu : IsFiniteEnergyCurve H J (ball 0 1 \ {0}) u) (P : ReebOrbit H)
    (Z : ℝ → CauchyRiemannIndex.Vec n →L[ℝ] V n) (hZ : IsUnitaryXiFrame J P Z)
    (Sinf : ℝ → CauchyRiemannIndex.Mat n) (hSinf : CauchyRiemannIndex.IsSymLoop Sinf)
    (hSinf' : ∀ i j, ContDiff ℝ ∞ (fun t => Sinf t i j))
    (hZS : ∀ η : ℝ → CauchyRiemannIndex.Vec n, ContDiff ℝ ∞ η → Function.Periodic η 1 →
      ∀ t : ℝ, asympOp J P (fun t => Z t (η t)) t =
        Z t (-(Matrix.toEuclideanLin (CauchyRiemannIndex.J₀ n) (deriv η t)) -
          Matrix.toEuclideanLin (Sinf t) (η t)))
    (ε : ℝ) (hε : ε = 1 ∨ ε = -1) (c : ℝ) (τ : ℝ × ℝ → ℝ) (h : ℝ × ℝ → V n) (s₀ : ℝ)
    (hτ : TendstoZeroCInfty (fun p : ℝ × ℝ => τ p - ε * P.T * p.2 - c))
    (hh : TendstoZeroCInfty h)
    (hrep : ∀ s ≥ s₀, ∀ t : ℝ,
      τ (s, t + 1) = τ (s, t) + ε * P.T ∧ h (s, t + 1) = h (s, t) ∧
        IsInXi H (P.x (τ (s, t))) (h (s, t)) ∧
        endW H u cylEnd (s, t) = proj H (P.x (τ (s, t)) + h (s, t)))
    (b C₀ : ℝ) (hb : 0 < b)
    (hdec : ∀ s ≥ s₀, ∀ t : ℝ,
      |τ (s, t) - ε * P.T * t - c| + ‖h (s, t)‖ ≤ C₀ * Real.exp (-(b * s))) :
    ∃ (s₁ d C : ℝ) (S : ℝ × ℝ → CauchyRiemannIndex.Mat n) (ζ : ℝ × ℝ → CauchyRiemannIndex.Vec n),
      0 < d ∧
      (∀ i j, ContDiffOn ℝ ∞ (fun p : ℝ × ℝ => S p i j) (Set.Ioi s₁ ×ˢ Set.univ)) ∧
      IsExpAsymptoticTo S (fun t => ε • Sinf (ε * t + c / P.T)) d ∧
      ContDiffOn ℝ ∞ ζ (Set.Ioi s₁ ×ˢ Set.univ) ∧
      ∀ s > s₁, ∀ t : ℝ, S (s, t + 1) = S (s, t) ∧ ζ (s, t + 1) = ζ (s, t) ∧
        CauchyRiemannIndex.crOp S ζ (s, t) = 0 ∧ h (s, t) = Z (τ (s, t) / P.T) (ζ (s, t)) ∧
        ‖ζ (s, t)‖ ≤ C * Real.exp (-(d * s)) := by
  sorry

end FiniteEnergyPlane
Source
Used for U. Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, J. Symplectic Geom. 12 (2014), arXiv:1105.2077, Theorem 2.11 and Lemma 2.12; H. Hofer, K. Wysocki, E. Zehnder, Properties of pseudoholomorphic curves in symplectisations I: asymptotics, Ann. Inst. H. Poincaré Anal. Non Linéaire 13 (1996)

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