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The weighted normal operator under a winding window is Fredholm of index zero

Proved
FiniteEnergyPlane.fredholm_index_zero_of_window

by Mazecto · Nov 12, 2026 · Mathlib 0df444a (Lean v4.33.1)

elliptic-pdefredholm-theorypseudoholomorphic-curves

Let S∞:R→R2×2S_\infty : \mathbb{R} \to \mathbb{R}^{2\times 2}S∞​:R→R2×2 be a smooth symmetric loop and δ∈R\delta \in \mathbb{R}δ∈R such that δ\deltaδ is not an eigenvalue of A∞=−J0∂t−S∞A_\infty = -J_0\partial_t - S_\inftyA∞​=−J0​∂t​−S∞​, eigenvalues μ<δ\mu < \deltaμ<δ have eigenfunctions of winding ≤0\le 0≤0 and eigenvalues μ>δ\mu > \deltaμ>δ have eigenfunctions of winding ≥1\ge 1≥1. Let S:R2→R2×2S : \mathbb{R}^2 \to \mathbb{R}^{2\times 2}S:R2→R2×2 be smooth, 111-periodic in ttt, exponentially asymptotic to S∞S_\inftyS∞​ at some rate d>0d > 0d>0 (IsExpAsymptoticTo), and of plane form (IsPlaneCoeff S: S(s,t)=4πzˉA(z)S(s,t) = 4\pi\bar z A(z)S(s,t)=4πzˉA(z), z=e2π(s+it)z = e^{2\pi(s+it)}z=e2π(s+it), AAA smooth on C\mathbb{C}C). Let χ\chiχ be smooth with χ′=π\chi' = \piχ′=π on (−∞,−1](-\infty,-1](−∞,−1] and χ′=δ\chi' = \deltaχ′=δ on [1,∞)[1,\infty)[1,∞) (IsSlopeWeight χ π δ), and write D=∂s+J0∂t+S+χ′(s)D = \partial_s + J_0\partial_t + S + \chi'(s)D=∂s​+J0​∂t​+S+χ′(s). Let 1<p<∞1 < p < \infty1<p<∞. Then D:W1,p→LpD : W^{1,p} \to L^pD:W1,p→Lp is Fredholm (IsFredholmCR) and its index is 000 (crIndex).

Role. The index count for the weighted normal operator along a holomorphic plane: the window at δ\deltaδ at the end s=+∞s = +\inftys=+∞ and the slope π\piπ at the removable end s=−∞s = -\inftys=−∞ balance to index 000. Combined with injectivity, this gives bijectivity.

Preamble
import Definitions.Def_FiniteEnergyPlane_TubeFamily
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology Set CauchyRiemannIndex
open scoped ContDiff ENNReal Real

/-- Under the same hypotheses on `Sinf`, `S` and `χ`, and for `1 < p < ∞`, the operator
`∂ₛ + J₀ ∂ₜ + S + χ' : W^{1,p} → L^p` is Fredholm of index `0`. -/
theorem fredholm_index_zero_of_window (p : ℝ≥0∞) [Fact (1 ≤ p)] (hp : 1 < p) (hp' : p ≠ ⊤)
    (Sinf : ℝ → Mat 1) (hSinf : IsSymLoop Sinf) (hSinf' : ∀ i j, ContDiff ℝ ∞ (fun t => Sinf t i j))
    (δ : ℝ) (hδe : ∀ e, ¬ IsLoopEigen Sinf δ e)
    (hwin : ∀ (μ : ℝ) (k : ℤ), HasLoopEigenWind Sinf μ k → (μ < δ ∧ k ≤ 0) ∨ (δ < μ ∧ 1 ≤ k))
    (S : ℝ × ℝ → Mat 1) (hS : ∀ i j, ContDiff ℝ ∞ (fun x : ℝ × ℝ => S x i j))
    (hSper : ∀ s t : ℝ, S (s, t + 1) = S (s, t))
    (d : ℝ) (hd : 0 < d) (hSas : IsExpAsymptoticTo S Sinf d) (hA : IsPlaneCoeff S)
    (χ : ℝ → ℝ) (hχ : IsSlopeWeight χ π δ) :
    IsFredholmCR p (fun x => S x + deriv χ x.1 • (1 : Mat 1)) ∧
      crIndex p (fun x => S x + deriv χ x.1 • (1 : Mat 1)) = 0 := by
  sorry

end FiniteEnergyPlane
Source
Toward U. Hryniewicz, Fast finite-energy planes in symplectizations and applications, Trans. AMS 364 (2012), arXiv:0812.4076, Lemmas 6.10 and 6.20; operators in the setting of C. Wendl, Lectures on Holomorphic Curves in Symplectic and Contact Geometry, arXiv:1011.1690, Ch. 4

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