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Weak LpL^pLp solutions of ∂sη+J0∂tη=f\partial_s\eta+J_0\partial_t\eta=f∂s​η+J0​∂t​η=f on the cylinder are graph-norm limits of test sections

Proved
CauchyRiemannIndex.weak_solution_graph_approx

by Mazecto · Oct 15, 2026 · Mathlib 0df444a (Lean v4.33.1)

cauchy-riemannsobolev-spacesweak-solutions

Let 1≤p<∞1\le p<\infty1≤p<∞, let J0=(0−IdId0)J_0=\begin{pmatrix}0&-\mathrm{Id}\\ \mathrm{Id}&0\end{pmatrix}J0​=(0Id​−Id0​) on R2n\mathbb R^{2n}R2n, and consider the cylinder R×S1\mathbb R\times S^1R×S1, S1=R/ZS^1=\mathbb R/\mathbb ZS1=R/Z, with coordinates (s,t)(s,t)(s,t). A test section is a smooth map φ:R×R→R2n\varphi:\mathbb R\times\mathbb R\to\mathbb R^{2n}φ:R×R→R2n that is 111-periodic in ttt and vanishes for ∣s∣|s|∣s∣ large. Let η,f∈Lp(R×S1,R2n)\eta,f\in L^p(\mathbb R\times S^1,\mathbb R^{2n})η,f∈Lp(R×S1,R2n) satisfy ∂sη+J0∂tη=f\partial_s\eta+J_0\partial_t\eta=f∂s​η+J0​∂t​η=f weakly, that is,

∫R×S1⟨−∂sφ+J0∂tφ, η⟩=∫R×S1⟨φ,f⟩for every test section φ.\int_{\mathbb R\times S^1}\big\langle-\partial_s\varphi+J_0\partial_t\varphi,\ \eta\big\rangle=\int_{\mathbb R\times S^1}\langle\varphi,f\rangle\qquad\text{for every test section }\varphi.∫R×S1​⟨−∂s​φ+J0​∂t​φ, η⟩=∫R×S1​⟨φ,f⟩for every test section φ.

Then for every ε>0\varepsilon>0ε>0 there is a test section uuu with

∥u−η∥Lp≤εand∥∂su+J0∂tu−f∥Lp≤ε.\|u-\eta\|_{L^p}\le\varepsilon\qquad\text{and}\qquad\|\partial_su+J_0\partial_tu-f\|_{L^p}\le\varepsilon.∥u−η∥Lp​≤εand∥∂s​u+J0​∂t​u−f∥Lp​≤ε.

So the weak extension of the constant-coefficient Cauchy–Riemann operator ∂s+J0∂t\partial_s+J_0\partial_t∂s​+J0​∂t​ on LpL^pLp coincides with the closure of its restriction to test sections. It is used for the W1,pW^{1,p}W1,p regularity of weak LpL^pLp solutions of Cauchy–Riemann type equations on the cylinder (Wendl, Proposition 4.6).

Formalization Note. R2n\mathbb R^{2n}R2n is Vec n === EuclideanSpace ℝ (Fin n ⊕ Fin n) and J0J_0J0​ is J₀ n, acting through Matrix.toEuclideanLin. Integrals over the cylinder are over the strip R×[0,1)\mathbb R\times[0,1)R×[0,1) (cylMeasure), and LpL^pLp is LpCyl n p with ppp in ℝ≥0∞, Fact (1 ≤ p) and p≠∞p\ne\inftyp=∞. Test sections are IsTestSection; ∂s,∂t\partial_s,\partial_t∂s​,∂t​ are partialS, partialT. The operator ∂su+J0∂tu\partial_su+J_0\partial_tu∂s​u+J0​∂t​u is written crOp (fun _ => 0) u, and ∥⋅∥Lp\|\cdot\|_{L^p}∥⋅∥Lp​ is eLpNorm with values in [0,∞][0,\infty][0,∞], as is ε\varepsilonε.

Preamble
import Definitions.Def_CauchyRiemannIndex_Setting
import Mathlib.Analysis.Calculus.ContDiff.Basic
import Mathlib.MeasureTheory.Integral.Bochner.Basic
Formal statement
namespace CauchyRiemannIndex

open MeasureTheory Matrix Filter Topology
open scoped ENNReal NNReal ContDiff RealInnerProductSpace

/-- Weak `L^p` solutions of `∂ₛη + J₀ ∂ₜη = f` on the cylinder are graph-norm limits of test
sections: if `η, f ∈ L^p` (`1 ≤ p < ∞`) and `∫ ⟨-∂ₛφ + J₀ ∂ₜφ, η⟩ = ∫ ⟨φ, f⟩` for every test
section `φ`, then for every `ε > 0` there is a test section `u` with `‖u - η‖_p ≤ ε` and
`‖∂ₛu + J₀ ∂ₜu - f‖_p ≤ ε`. -/
theorem weak_solution_graph_approx (n : ℕ) (p : ℝ≥0∞) [Fact (1 ≤ p)] (hp' : p ≠ ⊤)
    (η f : LpCyl n p)
    (hweak : ∀ φ : ℝ × ℝ → Vec n, IsTestSection φ →
      ∫ x, inner ℝ (-partialS φ x + Matrix.toEuclideanLin (J₀ n) (partialT φ x)) (η x)
          ∂cylMeasure = ∫ x, inner ℝ (φ x) (f x) ∂cylMeasure) :
    ∀ ε : ℝ≥0∞, 0 < ε → ∃ u : ℝ × ℝ → Vec n, IsTestSection u ∧
      eLpNorm (u - ⇑η) p cylMeasure ≤ ε ∧
      eLpNorm (crOp (fun _ : ℝ × ℝ => (0 : Mat n)) u - ⇑f) p cylMeasure ≤ ε := by
  sorry

end CauchyRiemannIndex
Source
C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, https://arxiv.org/abs/1612.01009, Lecture 4, Proposition 4.6, p. 70 (setting of the weak Cauchy-Riemann equation on the cylinder)

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