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Eventual coefficient bounds for a matrix field converging in C∞C^\inftyC∞ on a half-cylinder

Proved
FiniteEnergyPlane.halfCyl_coeff_bounds

by Mazecto · Oct 28, 2026 · Mathlib 0df444a (Lean v4.33.1)

asymptotic-operatorpseudoholomorphic-curvessymplectic-geometry

Let S:R×R→R2n×2nS:\mathbb{R}\times\mathbb{R}\to\mathbb{R}^{2n\times2n}S:R×R→R2n×2n be smooth, and let S∞:R→R2n×2nS_\infty:\mathbb{R}\to\mathbb{R}^{2n\times2n}S∞​:R→R2n×2n be a smooth symmetric 111-periodic loop. Suppose S(s,t)→S∞(t)S(s,t)\to S_\infty(t)S(s,t)→S∞​(t) in C∞C^\inftyC∞ as s→+∞s\to+\inftys→+∞, entrywise and uniformly in ttt. Then there are s0>0s_0>0s0​>0 and ccc such that for all s≥s0s\ge s_0s≥s0​, all ttt and all entries (i,j)(i,j)(i,j),

∣Sij(s,t)∣≤c,∣∂sSij(s,t)∣≤c,∣∂s2Sij(s,t)∣≤c.|S_{ij}(s,t)|\le c,\qquad|\partial_sS_{ij}(s,t)|\le c,\qquad|\partial_s^2S_{ij}(s,t)|\le c.∣Sij​(s,t)∣≤c,∣∂s​Sij​(s,t)∣≤c,∣∂s2​Sij​(s,t)∣≤c.

So the coefficients of the linear Cauchy–Riemann operator ∂s+J0∂t+S\partial_s+J_0\partial_t+S∂s​+J0​∂t​+S, and their first two sss-derivatives, are uniformly bounded far out on the half-cylinder.

Formalization Note The convergence is IsCInftyAsymptoticTo S Sinf. The sss-derivatives are written as fderiv ℝ (fun p => S p i j) (s, t) (1, 0) and fderiv ℝ (fun p => fderiv ℝ (fun q => S q i j) p (1, 0)) (s, t) (1, 0).

Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real RealInnerProductSpace

/-- If `S(s, t) → S∞(t)` in `C^∞` with `S∞` a smooth symmetric loop, then for large `s` the entries
of `S`, `∂ₛS` and `∂ₛ²S` are bounded by a fixed constant. -/
theorem halfCyl_coeff_bounds {n : ℕ} (S : ℝ × ℝ → CauchyRiemannIndex.Mat n)
    (hS : ∀ i j, ContDiff ℝ ∞ (fun p : ℝ × ℝ => S p i j))
    (Sinf : ℝ → CauchyRiemannIndex.Mat n) (hSinf : CauchyRiemannIndex.IsSymLoop Sinf)
    (hSinf' : ∀ i j, ContDiff ℝ ∞ (fun t => Sinf t i j))
    (hSas : IsCInftyAsymptoticTo S Sinf) :
    ∃ s₀ c : ℝ, 0 < s₀ ∧ ∀ s ≥ s₀, ∀ t : ℝ, ∀ i j, |S (s, t) i j| ≤ c ∧
      |fderiv ℝ (fun p : ℝ × ℝ => S p i j) (s, t) (1, 0)| ≤ c ∧
      |fderiv ℝ (fun p : ℝ × ℝ => fderiv ℝ (fun q : ℝ × ℝ => S q i j) p (1, 0)) (s, t) (1, 0)| ≤
        c := by
  sorry

end FiniteEnergyPlane
Source
Used for C. Wendl, Lectures on Symplectic Field Theory (2026 notes), Lemma 4.8.8

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