Floquet exceptional points and chirality in non-Hermitian Hamiltonians
arXiv:1710.04415 · doi:10.1088/1751-8121/aa931f
Abstract
Floquet exceptional points correspond to the coalescence of two (or more) quasi-energies and corresponding Floquet eigenstates of a time-periodic non-Hermitian Hamiltonian. They generally arise when the oscillation frequency satisfies a multiphoton resonance condition. Here we discuss the interplay between Floquet exceptional points and the chiral dynamics observed, over several oscillation cycles, in a wide class of non-Hermitian systems when they are slowly cycled in opposite directions of parameter space.
20 pages, 5 figures, submitted to J Phys A
References in corpus (10)
- Making Sense of Non-Hermitian Hamiltonians
- The physics of exceptional points
- Visualization of Branch Points in PT-Symmetric Waveguides
- Dynamically encircling exceptional points: Exact evolution and polarization state conversion
- A non-Hermitian symmetric Bose-Hubbard model: eigenvalue rings from unfolding higher-order exceptional points
- Invisibility and PT-symmetry
- Exceptional Points in Atomic Spectra
- Chirality of wave functions for three coalescing levels
- Geometric Phase for Non-Hermitian Hamiltonians and Its Holonomy Interpretation
- Non-Hermitian time-dependent perturbation theory: asymmetric transitions and transitionless interactions
Cited by in corpus (4)
- Floquet engineering of topological localization transitions and mobility edges in one-dimensional non-Hermitian quasicrystals
- Generalized bulk-boundary correspondence in periodically driven non-Hermitian systems
- Non-Hermitian Floquet phases with even-integer topological invariants in a periodically quenched two-leg ladder
- Complex Berry phase and imperfect non-Hermitian phase transitions