Connecting active and passive PT -symmetric Floquet modulation models
Abstract Open systems with gain, loss, or both, described by non-Hermitian Hamiltonians, have been a research frontier for the past decade. In particular, such Hamiltonians which possess parity-time (PT) symmetry feature dynamically stable regimes of unbroken symmetry with completely real eigenspectra that are rendered into complex conjugate pairs as the strength of the non-Hermiticity increases. By subjecting a PT-symmetric system to a periodic (Floquet) driving, the regime of dynamical stability can be dramatically affected, leading to a frequency-dependent threshold for the PT-symmetry breaking transition. We present a simple model of a time-dependent PT-symmetric Hamiltonian which smoothly connects the static case, a PT-symmetric Floquet case, and a neutral-PT-symmetric case. We analytically and numerically analyze the PT phase diagrams in each case, and show that slivers of PT-broken (PT-symmetric) phase extend deep into the nominally low (high) non-Hermiticity region.