paper

Power law hopping of single particles in one-dimensional non-Hermitian quasicrystals

arXiv:2301.09029 · doi:10.1103/PhysRevB.107.174205

Abstract

In this paper, a non-Hermitian Aubry-André-Harper model with power-law hoppings () and quasiperiodic parameter is studied, where is the power-law index, is the hopping distance, and is a member of the metallic mean family. We find that under the weak non-Hermitian effect, there preserves regimes where the fraction of ergodic eigenstates is -dependent as L ( is the system size) similar to those in the Hermitian case. However, regimes are ruined by the strong non-Hermitian effect. Moreover, by analyzing the fractal dimension, we find that there are two types of edges aroused by the power-law index in the single-particle spectrum, i.e., an ergodic-to-multifractal edge for the long-range hopping case (), and an ergodic-to-localized edge for the short-range hopping case (). Meanwhile, the existence of these two types of edges is found to be robust against the non-Hermitian effect. By employing the Simon-Spence theory, we analyzed the absence of the localized states for . For the short-range hopping case, with the Avila's global theory and the Sarnak method, we consider a specific example with to reveal the presence of the intermediate phase and to analytically locate the intermediate regime and the ergodic-to-multifractal edge, which are self-consistent with the numerically results.

8 pages, 8 figures

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