Quantum Entanglement of Non-Hermitian Quasicrystals
arXiv:2112.13411 · doi:10.1103/PhysRevB.105.L121115
Abstract
As a hallmark of pure quantum effect, quantum entanglement has provided unconventional routes to condensed matter systems. Here, from the perspective of quantum entanglement, we disclose exotic quantum physics in non-Hermitian quasicrystals. We present a class of experimentally realizable models for non-Hermitian quasicrystal chains, in which asymmetric hopping and complex potential coexist. We diagnose global phase diagram by means of entanglement from both real-space and momentum-space partition. By measuring entanglement entropy, we numerically determine the metal-insulator transition point. We combine real-space and momentum-space entanglement spectra to complementarily characterize the delocalization phase and the localization phase. Inspired by entanglement spectrum, we further analytically prove that a duality exists between the two phase regions. The transition point is self-dual and exact, further validating the numerical result from diagonalizing non-Hermitian matrices. Finally, we identify mobility edge by means of entanglement.
Accepted by Phys. Rev. B (Letter). New data in SM added, references updated
References in corpus (11)
- Anderson Transitions
- Entanglement Spectrum as a Generalization of Entanglement Entropy: Identification of Topological Order in Non-Abelian Fractional Quantum Hall Effect States
- Topological phase transition in non-Hermitian quasicrystals
- Entanglement Spectrum of a Disordered Topological Chern Insulator
- Phase transitions in a non-Hermitian Aubry-André-Harper model
- Quantum anomaly, non-Hermitian skin effects, and entanglement entropy in open systems
- Entanglement entropy and multifractality at localization transitions
- Free-fermion Entanglement Spectrum through Wannier Interpolation
- Dynamics of entanglement after exceptional quantum quench
- Position momentum Duality in the Entanglement Spectrum of Free Fermions
- Signatures of metal-insulator and topological phase transitions in the entanglement of one-dimensional disordered fermions