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Almost Mathieu operators with completely resonant phases

Spectral Theory 2021-11-03 v2 Mathematical Physics math.MP

Abstract

Let αR\Q\alpha\in \mathbb{R}\backslash \mathbb{Q} and β(α)=lim supn(lnqn+1)/qn<\beta(\alpha) = \limsup _{n \to \infty}(\ln q_{n+1})/ q_n <\infty, where pn/qnp_n/q_n is the continued fraction approximations to α\alpha. Let (Hλ,α,θu)(n)=u(n+1)+u(n1)+2λcos2π(θ+nα)u(n)(H_{\lambda,\alpha,\theta}u) (n)=u(n+1)+u(n-1)+ 2\lambda \cos2\pi(\theta+n\alpha)u(n) be the almost Mathieu operator on 2(Z)\ell^2(\mathbb{Z}), where λ,θR\lambda, \theta\in \mathbb{R}. Avila and Jitomirskaya \cite{avila2009ten} conjectured that for 2θαZ+Z2\theta \in \alpha \mathbb{Z} + \mathbb{Z}, Hλ,α,θH_{\lambda,\alpha,\theta} satisfies Anderson localization if λ>e2β(α)|\lambda|>e^{2\beta(\alpha)}. In this paper, we developed a method to treat simultaneous frequency and phase resonances and obtain that for 2θαZ+Z2\theta\in \alpha \mathbb{Z}+\mathbb{Z}, Hλ,α,θH_{\lambda,\alpha,\theta} satisfies Anderson localization if λ>e3β(α)|\lambda|>e^{3\beta(\alpha)}.

Cite

@article{arxiv.1805.01581,
  title  = {Almost Mathieu operators with completely resonant phases},
  author = {Wencai Liu},
  journal= {arXiv preprint arXiv:1805.01581},
  year   = {2021}
}

Comments

Ergodic Theory Dynam. Systems to appear

R2 v1 2026-06-23T01:44:46.580Z