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Exponential decay for linear Cauchy–Riemann equations on an end of a cylinder

Proved
FiniteEnergyPlane.halfCyl_exp_decay_eventually

by Mazecto · Oct 29, 2026 · Mathlib 0df444a (Lean v4.33.1)

asymptotic-analysispartial-differential-equationspseudoholomorphic-curves

Let s1∈Rs_1\in\mathbb{R}s1​∈R, let S(s,t)S(s,t)S(s,t) be real 2n×2n2n\times2n2n×2n matrices depending smoothly on (s,t)∈(s1,∞)×R(s,t)\in(s_1,\infty)\times\mathbb{R}(s,t)∈(s1​,∞)×R and 111-periodic in ttt there, and let S∞S_\inftyS∞​ be a smooth 111-periodic loop of symmetric matrices with S(s,t)→S∞(t)S(s,t)\to S_\infty(t)S(s,t)→S∞​(t) in C∞C^\inftyC∞, uniformly in ttt, as s→+∞s\to+\inftys→+∞. Suppose the asymptotic operator −J0∂t−S∞-J_0\partial_t-S_\infty−J0​∂t​−S∞​ is nondegenerate. Let ζ:R2→R2n\zeta:\mathbb{R}^2\to\mathbb{R}^{2n}ζ:R2→R2n be smooth on (s1,∞)×R(s_1,\infty)\times\mathbb{R}(s1​,∞)×R, 111-periodic in ttt there, with

∂sζ+J0∂tζ+Sζ=0(s>s1),\partial_s\zeta+J_0\partial_t\zeta+S\zeta=0\qquad(s>s_1),∂s​ζ+J0​∂t​ζ+Sζ=0(s>s1​),

and ζ(s,t)→0\zeta(s,t)\to0ζ(s,t)→0 uniformly in ttt. Then ζ\zetaζ decays exponentially: 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 all s≥s2s\ge s_2s≥s2​ and all ttt.

This is the exponential decay statement for linear Cauchy–Riemann equations on a half-cylinder in the form in which it is applied on an end, where the equation and its coefficients are only given for sss beyond some s1s_1s1​.

Formalization Note C∞C^\inftyC∞ convergence of matrices is entrywise IsCInftyAsymptoticTo; uniform convergence is TendstoZeroUnif. Mat n and Vec n are 2n×2n2n\times2n2n×2n real matrices and R2n\mathbb{R}^{2n}R2n, crOp S ζ is ∂sζ+J0∂tζ+Sζ\partial_s\zeta+J_0\partial_t\zeta+S\zeta∂s​ζ+J0​∂t​ζ+Sζ, a loop of symmetric matrices is IsSymLoop (continuous, 111-periodic, symmetric), and nondegeneracy of −J0∂t−S∞-J_0\partial_t-S_\infty−J0​∂t​−S∞​ is CauchyRiemannIndex.IsNondegenerate (111 is not an eigenvalue of the time-111 map Ψ(1)\Psi(1)Ψ(1) of Ψ′=J0S∞Ψ\Psi'=J_0S_\infty\PsiΨ′=J0​S∞​Ψ, Ψ(0)=1\Psi(0)=1Ψ(0)=1).

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`, with data
given only there: if `S` is smooth and `1`-periodic in `t` for `s > s₁`, `S(s, t) → S∞(t)` 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_eventually {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))
    (hSas : IsCInftyAsymptoticTo S Sinf) (hnd : CauchyRiemannIndex.IsNondegenerate Sinf)
    (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
C. Wendl, Lectures on Symplectic Field Theory (2026 notes), Proposition 6.7.1; H. Hofer, K. Wysocki, E. Zehnder, Ann. Inst. H. Poincaré Anal. Non Linéaire 13 (1996)

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