“…In particular, non-Hermitian couplings have been used to describe a PT -symmetric extension of the Lee model in the ghost regime 59,78,79 , non-Hermitian Bose-Hubbard Hamiltonians 80 , and PT -symmetric extensions of the Jaynes-Cumming model 81 . Effective models that yield non-Hermitian couplings are also encountered in the theory of the inverted quantum oscillators and quantum amplifiers 82,83 and introduced in several other systems 84,85,86,87,88,89,90,91 . In particular, engineered optical structures where photonic transport arises from evanescent field coupling can be tailored to simulate an effective non-Hermitian interaction between a discrete state (such as an optical resonator or waveguide) with a continuum of states (such as a chain of optical resonators, a waveguide array, a slab waveguide or a photonic crystal) 92,93 .…”