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      Metal-insulator phase transition in a non-Hermitian Aubry-Andr\'e-Harper Model

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          Abstract

          Non-Hermitian extensions of the Anderson and Aubry-Andr\'e-Harper models are attracting a considerable interest as platforms to study localization phenomena, metal-insulator and topological phase transitions in disordered non-Hermitian systems. Most of available studies, however, resort to numerical results, while few analytical and rigorous results are available owing to the extraordinary complexity of the underlying problem. Here we consider a parity-time (\(\mathcal{PT}\)) symmetric extension of the Aubry-Andr\'e-Harper model, undergoing a topological metal-insulator phase transition, and provide rigorous analytical results of energy spectrum, symmetry breaking phase transition and localization length. In particular, by extending to the non-Hermitian realm the Thouless\(^{\prime}\)s result relating localization length and density of states, we derive an analytical form of the localization length in the insulating phase, showing that -- like in the Hermitian Aubry-Andr\'e-Harper model-- the localization length is independent of energy.

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          Anatomy of skin modes and topology in non-Hermitian systems

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            Bandwidths for a quasiperiodic tight-binding model

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              New topological invariants in non-Hermitian systems

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                Author and article information

                Journal
                09 August 2019
                Article
                1908.03371
                d5ac4103-1643-4503-9356-83dc91bc7050

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                11 pages, 2 figures, comments are welcome
                quant-ph cond-mat.stat-mech

                Condensed matter,Quantum physics & Field theory
                Condensed matter, Quantum physics & Field theory

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