English

Kotani Theory for ergodic matrix-like Jacobi operators

Mathematical Physics 2021-05-26 v1 math.MP

Abstract

We extend the so-called Kotani Theory for a particular class of ergodic matrix-like Jacobi operators defined in l2(Z;Cl)l^{2}(\mathbb{Z}; \mathbb{C}^{l}) by the law [Hωu]n:=D(Tn1ω)un1+D(Tnω)un+1+V(Tnω)un[H_{\omega} \textbf{u}]_{n} := D^{*}(T^{n - 1}\omega) \textbf{u}_{n - 1} + D(T^{n}\omega) \textbf{u}_{n + 1} + V(T^{n}\omega) \textbf{u}_{n}, where T:ΩΩT: \Omega \rightarrow \Omega is an ergodic automorphism in the measure space (Ω,ν)(\Omega, \nu), the map D:ΩGL(l,R)D: \Omega \rightarrow GL(l, \mathbb{R}) is bounded, and for each ωΩ\omega\in\Omega, D(ω)D(\omega) is symmetric. Namely, it is shown that for each r{1,,l}r\in\{1,\ldots,l\}, the essential closure of Zr:={xR\mathcal{Z}_{r} := \{x \in \mathbb{R}\mid exactly 2r2r Lyapunov exponents of AzA_z are zero}\} coincides with σac,2r(Hω)\sigma_{ac,2r}(H_{\omega}), the absolutely continuous spectrum of multiplicity 2r2r, where AzA_z is a Schr\"odinger-like cocycle induced by HωH_\omega. Moreover, if k{1,,2l}k\in\{1,\ldots,2l\} is odd, then σac,k(Hω)=\sigma_{ac,k}(H_{\omega})=\emptyset for ν\nu-a.e. ωΩ\omega\in\Omega. We also provide a Thouless Formula for such class of operators.

Keywords

Cite

@article{arxiv.2105.11524,
  title  = {Kotani Theory for ergodic matrix-like Jacobi operators},
  author = {Fabrício Vieira Oliveira and Silas L. Carvalho},
  journal= {arXiv preprint arXiv:2105.11524},
  year   = {2021}
}
R2 v1 2026-06-24T02:25:20.324Z