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Kernel elements of cylinder Cauchy–Riemann operators are smooth

Proved
FiniteEnergyPlane.exists_smooth_of_crApply_eq_zero

by Mazecto · Nov 12, 2026 · Mathlib 0df444a (Lean v4.33.1)

elliptic-pdefredholm-theorypseudoholomorphic-curves

Let 2<p<∞2 < p < \infty2<p<∞ and let M:R2→R2×2M : \mathbb{R}^2 \to \mathbb{R}^{2\times 2}M:R2→R2×2 have C∞C^\inftyC∞ entries with M(s,t+1)=M(s,t)M(s, t+1) = M(s,t)M(s,t+1)=M(s,t). Let w=(w0,ws,wt)∈W1,pw = (w_0, w_s, w_t) \in W^{1,p}w=(w0​,ws​,wt​)∈W1,p (W1p p 1) on the cylinder satisfy

ws+J0wt+Mw0=0a.e.w_s + J_0 w_t + M w_0 = 0 \quad \text{a.e.}ws​+J0​wt​+Mw0​=0a.e.

(crApply M w =ᵐ 0). Then there is a C∞C^\inftyC∞ map g:R2→R2g : \mathbb{R}^2 \to \mathbb{R}^2g:R2→R2 with g(s,t+1)=g(s,t)g(s, t+1) = g(s,t)g(s,t+1)=g(s,t), w0=gw_0 = gw0​=g a.e., ∂sg+J0∂tg+Mg=0\partial_s g + J_0\partial_t g + M g = 0∂s​g+J0​∂t​g+Mg=0 everywhere (crOp M g = 0), and ∂sg,∂tg∈Lp\partial_s g, \partial_t g \in L^p∂s​g,∂t​g∈Lp on the cylinder.

Role. Elliptic regularity for kernel elements of Cauchy–Riemann type operators on the cylinder with smooth periodic coefficients, in the Sobolev setting of CauchyRiemannIndex. It turns a weak kernel element into a classical smooth solution with the same integrability.

Preamble
import Definitions.Def_FiniteEnergyPlane_TubeFamily
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology Set CauchyRiemannIndex
open scoped ContDiff ENNReal Real

/-- For `p > 2` and a smooth `1`-periodic coefficient `M`, every `w ∈ W^{1,p}` with
`(∂ₛ + J₀ ∂ₜ + M) w = 0` a.e. has a smooth `1`-periodic representative `g` of its first component
that solves `(∂ₛ + J₀ ∂ₜ + M) g = 0` everywhere, with `∂ₛ g, ∂ₜ g ∈ L^p` on the cylinder. -/
theorem exists_smooth_of_crApply_eq_zero (p : ℝ≥0∞) [Fact (1 ≤ p)] (hp : 2 < p) (hp' : p ≠ ⊤)
    (M : ℝ × ℝ → Mat 1) (hM : ∀ i j, ContDiff ℝ ∞ (fun x : ℝ × ℝ => M x i j))
    (hMper : ∀ s t : ℝ, M (s, t + 1) = M (s, t))
    (w : Triple 1 p) (hw : w ∈ W1p p 1) (h0 : crApply M w =ᵐ[cylMeasure] 0) :
    ∃ g : ℝ × ℝ → Vec 1, ContDiff ℝ ∞ g ∧ (∀ s t : ℝ, g (s, t + 1) = g (s, t)) ∧
      (w.1 : ℝ × ℝ → Vec 1) =ᵐ[cylMeasure] g ∧ (∀ x, crOp M g x = 0) ∧
      MemLp (partialS g) p cylMeasure ∧ MemLp (partialT g) p cylMeasure := by
  sorry

end FiniteEnergyPlane
Source
Toward U. Hryniewicz, Fast finite-energy planes in symplectizations and applications, Trans. AMS 364 (2012), arXiv:0812.4076, Lemmas 6.10 and 6.20; operators in the setting of C. Wendl, Lectures on Holomorphic Curves in Symplectic and Contact Geometry, arXiv:1011.1690, Ch. 4

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