Numerical calculation of the complex berry phase in non-Hermitian systems
arXiv:1708.03230 · doi:10.14311/AP.2017.57.0470
Abstract
We numerically investigate topological phases of periodic lattice systems in tight-binding description under the influence of dissipation. The effects of dissipation are effectively described by -symmetric potentials. In this framework we develop a general numerical gauge smoothing procedure to calculate complex Berry phases from the biorthogonal basis of the system's non-Hermitian Hamiltonian. Further, we apply this method to a one-dimensional -symmetric lattice system and verify our numerical results by an analytical calculation.
7 pages, 3 figures, minor modifications in the final version
References in corpus (10)
- Signatures of Majorana fermions in hybrid superconductor-semiconductor nanowire devices
- Colloquium: Majorana Fermions in nuclear, particle and solid-state physics
- Topological invariance and global Berry phase in non-Hermitian systems
- Mean-field dynamics of a non-Hermitian Bose-Hubbard dimer
- Topological phase in a non-Hermitian PT symmetric system
- Delta-Function Potential with a Complex Coupling
- Interface between Hermitian and non-Hermitian Hamiltonians in a model calculation
- Quantum master equation with balanced gain and loss
- Nonlinear PT-symmetric plaquettes
- An explicitly solvable model of the spontaneous PT-symmetry breaking
Cited by in corpus (5)
- Spontaneous topological pumping in non-Hermitian systems
- Topology of multipartite non-Hermitian one-dimensional systems
- Topological phases of commensurate or incommensurate non-Hermitian Su-Schrieffer-Heeger lattices
- Topological states at exceptional points
- Pseudo-Jahn-Teller interaction among electronic resonant states of H3