Topological Phases in a PT-Symmetric Dissipative Kitaev Chain
arXiv:2301.08446 · doi:10.7566/JPSCP.38.011165
Abstract
We study a topological phase in the dissipative Kitaev chain described by the Markovian quantum master equation. Based on the correspondence between Lindbladians, which generate the dissipative time-evolution, and non-Hermitian matrices, Lindbladians are classified in terms of non-Hermitian topological phases. We find out that the Lindbladian retains PT symmetry which is the prominent symmetry of open systems and then all the bulk modes can have a common lifetime. Moreover, when open boundary conditions are imposed on the system, the edge modes which break PT symmetry emerge, and one of the edge modes has a zero eigenvalue.
arXiv comment6 pages, 2 figures, accepted for publication in JPS Conference Proceedings (LT29)
References in corpus (12)
- Real Spectra in Non-Hermitian Hamiltonians Having PT Symmetry
- Symmetry and Topology in Non-Hermitian Physics
- Third quantization: a general method to solve master equations for quadratic open Fermi systems
- Metrology with -symmetric cavities: Enhanced sensitivity near the -phase transition
- Tenfold Way for Quadratic Lindbladians
- Parity-time-symmetric topological superconductor
- Spectral theorem for the Lindblad equation for quadratic open fermionic systems
- Topological phase in a non-Hermitian PT symmetric system
- PT-symmetric quantum Liouvillian dynamics
- Dynamical signatures of topological order in the driven-dissipative Kitaev chain
- Topological phases protected by shifted sublattice symmetry in dissipative quantum systems
- Bulk-edge correspondence and stability of multiple edge states of a symmetric non-Hermitian system by using non-unitary quantum walks