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Periodic solutions of J0ψ′+S∞ψ=gJ_0\psi'+S_\infty\psi=gJ0​ψ′+S∞​ψ=g for a nondegenerate asymptotic operator, with a uniform bound by ∥g∥L1\|g\|_{L^1}∥g∥L1​

Proved
CauchyRiemannIndex.exists_periodic_solution_bound

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

cauchy-riemannordinary-differential-equationssymplectic-geometry

Let S∞:R→R2n×2nS_\infty:\mathbb R\to\mathbb R^{2n\times2n}S∞​:R→R2n×2n be a continuous 111-periodic loop of symmetric matrices whose asymptotic operator A=−J0∂t−S∞(t)A=-J_0\partial_t-S_\infty(t)A=−J0​∂t​−S∞​(t) is nondegenerate, where J0=(0−Id Id0)J_0=\begin{pmatrix}0&-\mathrm{Id}\ \mathrm{Id}&0\end{pmatrix}J0​=(0​−Id Id​0​). Then there is a constant CCC, depending only on S∞S_\inftyS∞​, such that for every continuous 111-periodic g:R→R2ng:\mathbb R\to\mathbb R^{2n}g:R→R2n there is a continuously differentiable 111-periodic ψ:R→R2n\psi:\mathbb R\to\mathbb R^{2n}ψ:R→R2n with

J0ψ′(t)+S∞(t)ψ(t)=g(t)and∣ψ(t)∣≤C∫01∣g(τ)∣ dτfor all t∈R.J_0\psi'(t)+S_\infty(t)\psi(t)=g(t)\quad\text{and}\quad|\psi(t)|\le C\int_0^1|g(\tau)|\,d\tau\qquad\text{for all }t\in\mathbb R.J0​ψ′(t)+S∞​(t)ψ(t)=g(t)and∣ψ(t)∣≤C∫01​∣g(τ)∣dτfor all t∈R.

In other words, the periodic problem −Aψ=g-A\psi=g−Aψ=g is solvable for continuous right-hand sides, with an L1→L∞L^1\to L^\inftyL1→L∞ bound for the solution. Asymptotic operators are those of Wendl (3.10); the statement is used for the one-dimensional periodic problem underlying the translation-invariant Cauchy–Riemann operator ∂s+J0∂t+S∞(t)\partial_s+J_0\partial_t+S_\infty(t)∂s​+J0​∂t​+S∞​(t) on the cylinder (Wendl, Theorem 4.11).

Formalization Note. R2n\mathbb R^{2n}R2n is EuclideanSpace ℝ (Fin n ⊕ Fin n), J0J_0J0​ is Matrix.J, and matrices act through Matrix.toEuclideanLin. The loop is IsSymLoop (continuous, 111-periodic, symmetric values); 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). C1C^1C1 is ContDiff ℝ 1, ψ′\psi'ψ′ is deriv ψ, and ∫01\int_0^1∫01​ is the Bochner integral over Set.Ico 0 1. The constant CCC is chosen before ggg.

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

open MeasureTheory Matrix Filter Topology
open scoped ENNReal NNReal ContDiff RealInnerProductSpace

/-- Let `S∞` be a nondegenerate loop of symmetric matrices. There is a constant `C` such that for
every continuous `1`-periodic `g : ℝ → ℝ²ⁿ` there is a `C¹` `1`-periodic `ψ : ℝ → ℝ²ⁿ` with
`J₀ ψ' + S∞ ψ = g` and `|ψ(t)| ≤ C ∫₀¹ |g|` for all `t`. -/
theorem exists_periodic_solution_bound (n : ℕ) (Sinf : ℝ → Mat n) (hS : IsSymLoop Sinf)
    (hnd : IsNondegenerate Sinf) :
    ∃ C : ℝ, ∀ g : ℝ → Vec n, Continuous g → Function.Periodic g 1 →
      ∃ ψ : ℝ → Vec n, ContDiff ℝ 1 ψ ∧ Function.Periodic ψ 1 ∧
        (∀ t, Matrix.toEuclideanLin (J₀ n) (deriv ψ t) +
          Matrix.toEuclideanLin (Sinf t) (ψ t) = g t) ∧
        ∀ t, ‖ψ t‖ ≤ C * ∫ τ in Set.Ico (0 : ℝ) 1, ‖g τ‖ := by
  sorry

end CauchyRiemannIndex
Source
C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, https://arxiv.org/abs/1612.01009, Lecture 3, (3.10) (asymptotic operators) and Lecture 4, Theorem 4.11, p. 71 (setting of the translation-invariant operator)

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