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Exponential decay on an end for Cauchy–Riemann equations asymptotic to a loop along a drifting phase

Proved
FiniteEnergyPlane.halfCyl_exp_decay_of_drift

by Mazecto · Oct 30, 2026 · Mathlib 0df444a (Lean v4.33.1)

asymptotic-analysispartial-differential-equationspseudoholomorphic-curves

Let J0J_0J0​ be the standard complex structure on R2n\mathbb{R}^{2n}R2n and S∞:R→R2n×2nS_\infty:\mathbb{R}\to\mathbb{R}^{2n\times2n}S∞​:R→R2n×2n a smooth 111-periodic loop of symmetric matrices whose asymptotic operator −J0∂t−S∞-J_0\partial_t-S_\infty−J0​∂t​−S∞​ is nondegenerate. Let s1∈Rs_1\in\mathbb{R}s1​∈R and let S:R2→R2n×2nS:\mathbb{R}^2\to\mathbb{R}^{2n\times2n}S:R2→R2n×2n be smooth on (s1,∞)×R(s_1,\infty)\times\mathbb{R}(s1​,∞)×R with S(s,t+1)=S(s,t)S(s,t+1)=S(s,t)S(s,t+1)=S(s,t) there. Let φ:R2→R\varphi:\mathbb{R}^2\to\mathbb{R}φ:R2→R be a phase such that φ(s,t)−t\varphi(s,t)-tφ(s,t)−t is smooth for large sss and every derivative of order ≥1\ge1≥1 of φ(s,t)−t\varphi(s,t)-tφ(s,t)−t tends to 000 as s→+∞s\to+\inftys→+∞, uniformly in ttt (no limit of φ(s,t)−t\varphi(s,t)-tφ(s,t)−t is assumed). Suppose that each entry of

S(s,t)−S∞(φ(s,t))S(s,t)-S_\infty(\varphi(s,t))S(s,t)−S∞​(φ(s,t))

tends to 000 in C∞C^\inftyC∞ as s→+∞s\to+\inftys→+∞. If ζ\zetaζ is smooth on (s1,∞)×R(s_1,\infty)\times\mathbb{R}(s1​,∞)×R, 111-periodic in ttt, solves ∂sζ+J0∂tζ+Sζ=0\partial_s\zeta+J_0\partial_t\zeta+S\zeta=0∂s​ζ+J0​∂t​ζ+Sζ=0 there, and ζ→0\zeta\to0ζ→0 uniformly in ttt, then there are δ>0\delta>0δ>0, CCC and s2s_2s2​ with ∥ζ(s,t)∥≤Ce−δs\|\zeta(s,t)\|\le Ce^{-\delta s}∥ζ(s,t)∥≤Ce−δs for s≥s2s\ge s_2s≥s2​.

This is the form needed for the normal component of a pseudoholomorphic end in tube coordinates around a nondegenerate periodic Reeb orbit, before the convergence of the asymptotic phase is known. With a constant phase φ(s,t)=t+c\varphi(s,t)=t+cφ(s,t)=t+c it reduces to halfCyl_exp_decay_eventually (8ec20b66).

Formalization Note "Tends to 000 in C∞C^\inftyC∞" is TendstoZeroCInfty; derivatives of φ(s,t)−t\varphi(s,t)-tφ(s,t)−t are iteratedFDeriv ℝ m (fun p => φ p - p.2). The equation is CauchyRiemannIndex.crOp S ζ (s, t) = 0.

Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Exponential decay for linear Cauchy–Riemann equations on an end `(s₁, ∞) × ℝ/ℤ` whose
coefficient is asymptotic to a nondegenerate loop along a drifting phase: if `S` is smooth and
`1`-periodic in `t` for `s > s₁`, `φ(s, t) - t` is smooth for large `s` with every derivative of
order `≥ 1` tending to `0` uniformly, `S(s, t) - S∞(φ(s, t)) → 0` in `C^∞`, the asymptotic operator
`-J₀ ∂ₜ - S∞` is nondegenerate, and the `1`-periodic smooth solution `ζ` of
`∂ₛζ + J₀ ∂ₜζ + S ζ = 0` on `s > s₁` tends to `0` uniformly, then `ζ` decays exponentially. -/
theorem halfCyl_exp_decay_of_drift {n : ℕ} (s₁ : ℝ) (S : ℝ × ℝ → CauchyRiemannIndex.Mat n)
    (hS : ∀ i j, ContDiffOn ℝ ∞ (fun p : ℝ × ℝ => S p i j) (Set.Ioi s₁ ×ˢ Set.univ))
    (Sinf : ℝ → CauchyRiemannIndex.Mat n) (hSinf : CauchyRiemannIndex.IsSymLoop Sinf)
    (hSinf' : ∀ i j, ContDiff ℝ ∞ (fun t => Sinf t i j))
    (hnd : CauchyRiemannIndex.IsNondegenerate Sinf) (φ : ℝ × ℝ → ℝ)
    (hφs : ∃ s₂ : ℝ, ContDiffOn ℝ ∞ (fun p : ℝ × ℝ => φ p - p.2) (Set.Ioi s₂ ×ˢ Set.univ))
    (hφ : ∀ m : ℕ, 1 ≤ m → ∀ η > 0, ∃ s₂ : ℝ, ∀ s ≥ s₂, ∀ t : ℝ,
      ‖iteratedFDeriv ℝ m (fun p : ℝ × ℝ => φ p - p.2) (s, t)‖ ≤ η)
    (hSas : ∀ i j, TendstoZeroCInfty (fun p : ℝ × ℝ => S p i j - Sinf (φ p) i j))
    (ζ : ℝ × ℝ → CauchyRiemannIndex.Vec n) (hζ : ContDiffOn ℝ ∞ ζ (Set.Ioi s₁ ×ˢ Set.univ))
    (hper : ∀ s > s₁, ∀ t : ℝ, S (s, t + 1) = S (s, t) ∧ ζ (s, t + 1) = ζ (s, t))
    (heq : ∀ s > s₁, ∀ t : ℝ, CauchyRiemannIndex.crOp S ζ (s, t) = 0)
    (hζ0 : TendstoZeroUnif ζ) :
    ∃ δ > 0, ∃ C s₂ : ℝ, ∀ s ≥ s₂, ∀ t : ℝ, ‖ζ (s, t)‖ ≤ C * Real.exp (-(δ * s)) := by
  sorry

end FiniteEnergyPlane
Source
H. Hofer, K. Wysocki, E. Zehnder, Properties of pseudoholomorphic curves in symplectisations I: asymptotics, Ann. Inst. H. Poincaré Anal. Non Linéaire 13 (1996), Section 2

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