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Coercive estimate, up to one direction per positive zero, for a Cauchy–Riemann operator with a large antilinear term

Proved
CauchyRiemannIndex.large_antilinear_coercive_estimate

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

analysiscauchy-riemann-operatorspde

Identify R2\mathbb R^2R2 with C\mathbb CC 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). Let β:R×R→C\beta:\mathbb R\times\mathbb R\to\mathbb Cβ:R×R→C be smooth and 111-periodic in ttt, with bounded derivative, and assume there are R,c>0R,c>0R,c>0 with c≤∣β(s,t)∣≤1/cc\le|\beta(s,t)|\le 1/cc≤∣β(s,t)∣≤1/c for ∣s∣≥R|s|\ge R∣s∣≥R. Let Z+,Z−⊂R×[0,1)Z^+,Z^-\subset\mathbb R\times[0,1)Z+,Z−⊂R×[0,1) be disjoint finite sets such that the zeros of β\betaβ are exactly the points (ζ1,ζ2+m)(\zeta_1,\zeta_2+m)(ζ1​,ζ2​+m), ζ∈Z+∪Z−\zeta\in Z^+\cup Z^-ζ∈Z+∪Z−, m∈Zm\in\mathbb Zm∈Z, and let r>0r>0r>0 be such that for ∣z∣<r|z|<r∣z∣<r

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

For σ∈R\sigma\in\mathbb Rσ∈R put

Dση=∂sη+i ∂tη+σ β ηˉ.D_\sigma\eta=\partial_s\eta+i\,\partial_t\eta+\sigma\,\beta\,\bar\eta .Dσ​η=∂s​η+i∂t​η+σβηˉ​.

Then there are constants AAA and σ0>0\sigma_0>0σ0​>0 such that for every σ≥σ0\sigma\ge\sigma_0σ≥σ0​ there exist smooth functions Φζ:R×R→C\Phi_\zeta:\mathbb R\times\mathbb R\to\mathbb CΦζ​:R×R→C (ζ∈Z+\zeta\in Z^+ζ∈Z+), 111-periodic in ttt and vanishing for large ∣s∣|s|∣s∣, with

∥η∥L22  ≤  Aσ ∥Dση∥L22+∑ζ∈Z+⟨Φζ,η⟩L22\|\eta\|_{L^2}^2\;\le\;\frac{A}{\sigma}\,\|D_\sigma\eta\|_{L^2}^2+\sum_{\zeta\in Z^+}\langle\Phi_\zeta,\eta\rangle_{L^2}^2∥η∥L22​≤σA​∥Dσ​η∥L22​+ζ∈Z+∑​⟨Φζ​,η⟩L22​

for every smooth η:R×R→C\eta:\mathbb R\times\mathbb R\to\mathbb Cη:R×R→C that is 111-periodic in ttt and vanishes for large ∣s∣|s|∣s∣. Here L2L^2L2 norms and real inner products ⟨u,v⟩=∫Re(uvˉ)\langle u,v\rangle=\int\mathrm{Re}(u\bar v)⟨u,v⟩=∫Re(uvˉ) are taken over R×[0,1)\mathbb R\times[0,1)R×[0,1).

This is a quantitative injectivity statement for DσD_\sigmaDσ​ at large σ\sigmaσ: apart from at most #Z+\#Z^+#Z+ directions, ∥Dση∥\|D_\sigma\eta\|∥Dσ​η∥ dominates σ ∥η∥\sqrt{\sigma}\,\|\eta\|σ​∥η∥. It is the analytic input for the bound dim⁡ker⁡Dσ≤#Z+\dim\ker D_\sigma\le\#Z^+dimkerDσ​≤#Z+ in Wendl's Lemma 5.22 and in the index computation of Proposition 5.27.

Formalization Note. Sections are maps ℝ × ℝ → Vec 1 (Vec 1 = ℝ²) satisfying IsTestSection; DσD_\sigmaDσ​ is crOp (fun x => σ • antilinearMat (β x)), where antilinearMat β is the real matrix of z↦βzˉz\mapsto\beta\bar zz↦βzˉ; integrals are over cylMeasure (Lebesgue measure on R×[0,1)\mathbb R\times[0,1)R×[0,1)). The functions Φζ\Phi_\zetaΦζ​ are given as a family Φ : ℝ × ℝ → ℝ × ℝ → Vec 1 of which only the members with ζ ∈ Zplus are used.

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

/-- A coercive estimate for a Cauchy–Riemann operator with a large antilinear term (Wendl,
Lecture 5, setting of § 5.5). Let `β : ℝ × S¹ → ℂ` be smooth and `1`-periodic in `t`, with bounded
derivative and with `|β|` bounded below for large `|s|`; let its zeros (mod `t ↦ t + 1`) be the
finite sets `Z⁺` and `Z⁻`, with `β(ζ + z) = z` for `ζ ∈ Z⁺` and `β(ζ + z) = z̄` for `ζ ∈ Z⁻` on the
disc `|z| < r`. Then there are `A` and `σ₀ > 0` such that for every `σ ≥ σ₀` there are smooth
compactly supported sections `Φ_ζ` (`ζ ∈ Z⁺`) with
`‖η‖²_{L²} ≤ (A/σ) ‖∂ₛη + J₀∂ₜη + σ β η̄‖²_{L²} + Σ_{ζ ∈ Z⁺} ⟨Φ_ζ, η⟩²_{L²}`
for every test section `η` of the cylinder. -/
theorem large_antilinear_coercive_estimate (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)
    (hminusZ : ∀ ζ ∈ Zminus, ∀ z : ℂ, ‖z‖ < r → β (ζ.1 + z.re, ζ.2 + z.im) = (starRingEnd ℂ) z) :
    ∃ A σ₀ : ℝ, 0 < σ₀ ∧ ∀ σ ≥ σ₀, ∃ Φ : ℝ × ℝ → ℝ × ℝ → Vec 1,
      (∀ ζ ∈ Zplus, IsTestSection (Φ ζ)) ∧
      ∀ η : ℝ × ℝ → Vec 1, IsTestSection η →
        ∫ x, ‖η x‖ ^ 2 ∂cylMeasure ≤
          A / σ * ∫ x, ‖crOp (fun x => σ • antilinearMat (β x)) η x‖ ^ 2 ∂cylMeasure +
            ∑ ζ ∈ Zplus, (∫ x, ⟪Φ ζ x, η x⟫ ∂cylMeasure) ^ 2 := by
  sorry

end CauchyRiemannIndex
Source
C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, Lecture 5, § 5.5 (setting of Lemma 5.22)

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