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Kernel dimension bound for Cauchy–Riemann operators with a large antilinear zeroth-order term

Proved
CauchyRiemannIndex.large_antilinear_kernel_le

by Mazecto · Oct 17, 2026 · Mathlib 0df444a (Lean v4.33.1)

cauchy-riemannfredholm-indexsobolev-spacessymplectic-geometry

Let n=1n=1n=1, let S±S^\pmS± be continuous loops of symmetric 2×22\times22×2 matrices with nondegenerate asymptotic operators, and let S:R×S1→R2×2S:\mathbb{R}\times S^1\to\mathbb{R}^{2\times2}S:R×S1→R2×2 be continuous with S(s,⋅)→S±S(s,\cdot)\to S^\pmS(s,⋅)→S± uniformly as s→±∞s\to\pm\inftys→±∞. Let β:R×S1→C\beta:\mathbb{R}\times S^1\to\mathbb{C}β:R×S1→C be smooth with bounded first derivative, such that ∣β∣|\beta|∣β∣ and 1/∣β∣1/|\beta|1/∣β∣ are bounded for large ∣s∣|s|∣s∣, and such that its zeros form finite sets Z+Z^+Z+ (positive zeros) and Z−Z^-Z− (negative zeros) with the following normal form: for some r>0r>0r>0 and every ζ∈Z±\zeta\in Z^\pmζ∈Z±, on the disc ∣z∣<r|z|<r∣z∣<r around ζ\zetaζ one has S=0S=0S=0 and

β(ζ+z)=z  (ζ∈Z+),β(ζ+z)=zˉ  (ζ∈Z−).\beta(\zeta+z)=z\ \ (\zeta\in Z^+),\qquad\beta(\zeta+z)=\bar z\ \ (\zeta\in Z^-).β(ζ+z)=z  (ζ∈Z+),β(ζ+z)=zˉ  (ζ∈Z−).

For σ>0\sigma>0σ>0 let Dση=∂sη+J0∂tη+Sη+σβηˉD_\sigma\eta=\partial_s\eta+J_0\partial_t\eta+S\eta+\sigma\beta\bar\etaDσ​η=∂s​η+J0​∂t​η+Sη+σβηˉ​, acting from W1,2W^{1,2}W1,2 to L2L^2L2.

Then there is σ0\sigma_0σ0​ such that for all σ≥σ0\sigma\ge\sigma_0σ≥σ0​ the kernel of DσD_\sigmaDσ​ is finite-dimensional and

dim⁡ker⁡Dσ≤#Z+.\dim\ker D_\sigma\le\#Z^+.dimkerDσ​≤#Z+.

This is the kernel half of Wendl's Lemma 5.22; together with the cokernel bound and the two matching lower bounds it gives the kernel and cokernel of DσD_\sigmaDσ​ for large σ\sigmaσ.

Formalization Note C=R2\mathbb{C}=\mathbb{R}^2C=R2 via (x,y)↦x+iy(x,y)\mapsto x+iy(x,y)↦x+iy, and η↦βηˉ\eta\mapsto\beta\bar\etaη↦βηˉ​ is the matrix antilinearMat β, so DσD_\sigmaDσ​ is DSσD_{S_\sigma}DSσ​​ with Sσ=S+σ⋅S_\sigma=S+\sigma\cdotSσ​=S+σ⋅antilinearMat ∘ β. Points of the cylinder are pairs (s,t)(s,t)(s,t) and ζ+z\zeta+zζ+z means (ζs+Re⁡z,ζt+Im⁡z)(\zeta_s+\operatorname{Re}z,\zeta_t+\operatorname{Im}z)(ζs​+Rez,ζt​+Imz); β\betaβ is 111-periodic in ttt, the zeros are listed in R×[0,1)\mathbb{R}\times[0,1)R×[0,1), and every zero of β\betaβ is a ttt-translate by an integer of a listed one. The hypotheses are those of the milestone CauchyRiemannIndex.large_antilinear_perturbation_index (Wendl, Proposition 5.27, with the assumptions of § 5.5); the chart near each zero is a translation of the coordinates (s,t)(s,t)(s,t), the trivialization is the global one, and the area form is ds dtds\,dtdsdt. The exponent is p=2p=2p=2. The conclusion is stated with FiniteDimensional and finrank of crKernel 2 ….

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

open MeasureTheory Matrix Filter Topology
open scoped ENNReal NNReal ContDiff RealInnerProductSpace

/-- Wendl, Lemma 5.22 (p. 97), kernel part, with the assumptions of § 5.5 (p. 94), on the cylinder
with the trivial line bundle and `p = 2`: let `D_S` (`n = 1`) be asymptotic to nondegenerate loops `S±` of symmetric
matrices, and let `β : ℝ × S¹ → ℂ` be smooth with bounded derivative, with `|β|` and `1/|β|`
bounded for large `|s|`, whose zeros (mod `t ↦ t + 1`) are the finite sets `Z⁺` (positive zeros) and
`Z⁻` (negative zeros), such that on a disc of radius `r` around each zero `ζ` the operator is `∂̄`
(`S = 0`) and `β(ζ + z) = z` for `ζ ∈ Z⁺`, `β(ζ + z) = z̄` for `ζ ∈ Z⁻`. Put
`D_σ η = D_S η + σ β η̄`. Then for all large `σ`, the kernel of
`D_σ : W^{1,2} → L²` is finite-dimensional of dimension at most `#Z⁺`. -/
theorem large_antilinear_kernel_le (Splus Sminus : ℝ → Mat 1) (hSplus : IsSymLoop Splus)
    (hSminus : IsSymLoop Sminus) (hplus : IsNondegenerate Splus) (hminus : IsNondegenerate Sminus)
    (S : ℝ × ℝ → Mat 1) (hS : IsAsymptoticTo S Splus Sminus)
    (β : ℝ × ℝ → ℂ) (hβ : ContDiff ℝ ∞ β) (hβper : ∀ s t, β (s, t + 1) = β (s, t))
    (hβC1 : ∃ C : ℝ, ∀ x, ‖fderiv ℝ β x‖ ≤ C)
    (hβends : ∃ (R c : ℝ), 0 < c ∧ ∀ s t, R ≤ |s| → c ≤ ‖β (s, t)‖ ∧ ‖β (s, t)‖ ≤ 1 / c)
    (Zplus Zminus : Finset (ℝ × ℝ)) (hZ : ∀ ζ ∈ Zplus ∪ Zminus, 0 ≤ ζ.2 ∧ ζ.2 < 1)
    (hdisj : Disjoint Zplus Zminus)
    (hzero : ∀ x : ℝ × ℝ, β x = 0 ↔ ∃ ζ ∈ Zplus ∪ Zminus, ∃ m : ℤ, x = (ζ.1, ζ.2 + m))
    (r : ℝ) (hr : 0 < r)
    (hplusZ : ∀ ζ ∈ Zplus, ∀ z : ℂ, ‖z‖ < r →
      β (ζ.1 + z.re, ζ.2 + z.im) = z ∧ S (ζ.1 + z.re, ζ.2 + z.im) = 0)
    (hminusZ : ∀ ζ ∈ Zminus, ∀ z : ℂ, ‖z‖ < r →
      β (ζ.1 + z.re, ζ.2 + z.im) = (starRingEnd ℂ) z ∧ S (ζ.1 + z.re, ζ.2 + z.im) = 0) :
    ∃ σ₀ : ℝ, ∀ σ ≥ σ₀,
      FiniteDimensional ℝ (crKernel 2 (fun x => S x + σ • antilinearMat (β x))) ∧
      Module.finrank ℝ (crKernel 2 (fun x => S x + σ • antilinearMat (β x))) ≤ Zplus.card := by
  sorry

end CauchyRiemannIndex
Source
C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, https://arxiv.org/abs/1612.01009, Lecture 5, Lemma 5.22, p. 97, with the assumptions of § 5.5, p. 94 (cylinder, trivial line bundle, p = 2)

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