Hermitian--to--quasi-Hermitian quantum phase transitions
arXiv:1804.03425 · doi:10.1103/PhysRevA.97.042117
Abstract
The phenomenon of quantum phase transition is considered in the special case in which the evolution laws remain unitary and in which the bound-state energies remain observable. The conventional Hermiticity of observables is lost at the interface, replaced by the so called quasi-Hermiticity. Several features of the passage of the system through the interface are discussed and illustrated by elementary illustrative symmetric examples.
24 pp., 5 figures
References in corpus (12)
- Making Sense of Non-Hermitian Hamiltonians
- The ODE/IM Correspondence
- Invisibility and PT-symmetry
- Time-dependent version of cryptohermitian quantum theory
- Three-Hilbert-Space Formulation of Quantum Mechanics
- Closed formula for the metric in the Hilbert space of a PT-symmetric model
- Resonances in open quantum systems
- Interface between Hermitian and non-Hermitian Hamiltonians in a model calculation
- Exact analytical solutions for time-dependent Hermitian Hamiltonian systems from static unobservable non-Hermitian Hamiltonians
- Non-Hermitian Heisenberg representation
- Tunable waveguide lattices with non-uniform parity-symmetric tunneling
- Three solvable matrix models of a quantum catastrophe