Non-Hermitian topological phase transitions in superlattices and the optical Dirac equation
arXiv:2109.01325 · doi:10.1364/OL.440052
Abstract
Optical superlattices with sublattice symmetry subjected to a synthetic imaginary gauge field undergo a topological phase transition in the Bloch energy spectrum, characterized by the change of a spectral winding number. For a narrow gap, the phase transition is of universal form and described by a non-Hermitian Dirac equation with Lorentz-symmetry violation. A simple photonic system displaying such a phase transition is discussed, which is based on light coupling in co-propagating gratings.
5 pages, 4 figures
References in corpus (8)
- Topological Origin of Non-Hermitian Skin Effects
- Efficient Light Funneling based on the non-Hermitian Skin Effect
- Topological phases in the non-Hermitian Su-Schrieffer-Heeger model
- Observation of arbitrary topological windings of a non-Hermitian band
- Observation of non-Bloch parity-time symmetry and exceptional points
- Topology of anti-parity-time-symmetric non-Hermitian Su-Schrieffer-Heeger model
- Non-Hermitian generalizations of extended Su-Schrieffer-Heeger models
- Foldy-Wouthuysen transformation for non-Hermitian Hamiltonians
Cited by in corpus (5)
- Topological photonic crystals: physics, designs and applications
- Non-Hermitian skin effect and self-acceleration
- Non-Hermitian skin effect beyond the tight-binding models
- Investigation of a non-Hermitian edge burst with time-dependent perturbation theory
- Self-healing of non-Hermitian topological skin modes