Generalized Lieb's theorem for noninteracting non-Hermitian n-partite tight-binding lattices

A. M. Marques and R. G. Dias
Phys. Rev. B 106, 205146 – Published 28 November 2022

Abstract

Hermitian bipartite models are characterized by the presence of chiral symmetry and by Lieb's theorem, which derives the number of zero-energy flat bands of the model from the imbalance of sites between its two sublattices. Here, we introduce a class of non-Hermitian models with an arbitrary number of sublattices connected in a unidirectional and cyclical way and show that the number of zero-energy flat bands of these models can be found from a generalized version of Lieb's theorem, in what regards its application to noninteracting tight-binding models, involving the imbalance between each sublattice and the sublattice of lowest dimension. Furthermore, these models are also shown to obey a generalized chiral symmetry, of the type found in the context of certain clock or parafermionic systems. The main results are illustrated with a simple toy model and possible realizations in different platforms of the models introduced here are discussed.

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  • Received 23 May 2022
  • Revised 28 October 2022
  • Accepted 15 November 2022

DOI:https://doi.org/10.1103/PhysRevB.106.205146

©2022 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

A. M. Marques* and R. G. Dias

  • Department of Physics & i3N, University of Aveiro, 3810-193 Aveiro, Portugal

  • *anselmomagalhaes@ua.pt

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Issue

Vol. 106, Iss. 20 — 15 November 2022

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