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Slab-wise L2L^2L2 amalgam bound for translation-invariant Cauchy–Riemann operators with nondegenerate asymptotics, p≥2p\ge2p≥2

Proved
CauchyRiemannIndex.translationInvariant_slab_L2_bound

by Mazecto · Oct 14, 2026 · Mathlib 0df444a (Lean v4.33.1)

cauchy-riemannelliptic-estimatessymplectic-geometry

Let 2≤p<∞2\le p<\infty2≤p<∞ and let S∞S_\inftyS∞​ be a continuous 111-periodic loop of symmetric 2n×2n2n\times2n2n×2n matrices whose asymptotic operator −J0∂t−S∞(t)-J_0\partial_t-S_\infty(t)−J0​∂t​−S∞​(t) is nondegenerate. Write D=∂s+J0∂t+S∞(t)D=\partial_s+J_0\partial_t+S_\infty(t)D=∂s​+J0​∂t​+S∞​(t) for the translation-invariant Cauchy–Riemann operator on the cylinder R×S1\mathbb R\times S^1R×S1. Then there is a constant K≥0K\ge0K≥0 such that

∫R(∫[s,s+1]×S1∣u∣2)p/2ds  ≤  K∫R×S1∣Du∣p\int_{\mathbb R}\Big(\int_{[s,s+1]\times S^1}|u|^2\Big)^{p/2}ds\;\le\;K\int_{\mathbb R\times S^1}|Du|^p∫R​(∫[s,s+1]×S1​∣u∣2)p/2ds≤K∫R×S1​∣Du∣p

for every smooth u:R×S1→R2nu:\mathbb R\times S^1\to\mathbb R^{2n}u:R×S1→R2n that vanishes for large ∣s∣|s|∣s∣.

The left side is the ppp-th power of the ℓp(L2)\ell^p(L^2)ℓp(L2) amalgam norm of uuu over unit slabs of the cylinder. The statement is a zero-order a priori bound for DDD (Wendl, Theorem 4.11, case k=1k=1k=1), in a form that is weaker than the LpL^pLp norm for p>2p>2p>2; it is used for the bound ∥u∥Lp≤c∥Du∥Lp\|u\|_{L^p}\le c\|Du\|_{L^p}∥u∥Lp​≤c∥Du∥Lp​.

Formalization Note. S1=R/ZS^1=\mathbb R/\mathbb ZS1=R/Z; maps on the cylinder are maps of (s,t)∈R2(s,t)\in\mathbb R^2(s,t)∈R2 that are 111-periodic in ttt, integrals over R×S1\mathbb R\times S^1R×S1 are over the strip R×[0,1)\mathbb R\times[0,1)R×[0,1) (cylMeasure), and the slab [s,s+1]×S1[s,s+1]\times S^1[s,s+1]×S1 is Set.Icc s (s + 1) ×ˢ Set.Ico 0 1 with Lebesgue measure. All integrals are lower Lebesgue integrals of ‖·‖ₑ powers, so no integrability is assumed. Test sections are IsTestSection (smooth, 111-periodic in ttt, zero for large ∣s∣|s|∣s∣); the operator is crOp with S(s,t)=S∞(t)S(s,t)=S_\infty(t)S(s,t)=S∞​(t). The loop is IsSymLoop; nondegeneracy is IsNondegenerate (det⁡(1−Ψ(1))≠0\det(1-\Psi(1))\ne0det(1−Ψ(1))=0 for the fundamental solution Ψ′=J0S∞Ψ\Psi'=J_0S_\infty\PsiΨ′=J0​S∞​Ψ, Ψ(0)=1\Psi(0)=1Ψ(0)=1). ppp is a real number with 2≤p2\le p2≤p; K∈R≥0K\in\mathbb R_{\ge0}K∈R≥0​ does not depend on uuu.

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

open MeasureTheory Matrix Filter Topology
open scoped ENNReal NNReal ContDiff RealInnerProductSpace

/-- Let `2 ≤ p < ∞` and let `S∞` be a nondegenerate loop of symmetric matrices. There is a
constant `K` such that every test section `u` of the cylinder `ℝ × S¹` satisfies
`∫_ℝ (∫_{[s, s+1] × [0,1)} |u|²)^{p/2} ds ≤ K ∫_{ℝ × [0,1)} |D u|^p`,
where `D = ∂ₛ + J₀ ∂ₜ + S∞(t)` is the translation-invariant Cauchy–Riemann operator.

The left side is the `p/2`-th power amalgam norm of `u` over the unit slabs of the cylinder. -/
theorem translationInvariant_slab_L2_bound (n : ℕ) (p : ℝ) (hp : 2 ≤ p)
    (Sinf : ℝ → Mat n) (hS : IsSymLoop Sinf) (hnd : IsNondegenerate Sinf) :
    ∃ K : ℝ≥0, ∀ u : ℝ × ℝ → Vec n, IsTestSection u →
      (∫⁻ s : ℝ, (∫⁻ x in Set.Icc s (s + 1) ×ˢ Set.Ico (0 : ℝ) 1, ‖u x‖ₑ ^ (2 : ℝ)) ^ (p / 2)) ≤
        K * ∫⁻ x, ‖crOp (fun x : ℝ × ℝ => Sinf x.2) u x‖ₑ ^ p ∂cylMeasure := by
  sorry

end CauchyRiemannIndex
Source
C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, https://arxiv.org/abs/1612.01009, Lecture 4, Theorem 4.11, p. 71 (setting of the translation-invariant operator, case k = 1)

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