Floquet resonant states and validity of the Floquet-Magnus expansion in the periodically driven Friedrichs models
arXiv:1412.6738 · doi:10.1103/PhysRevA.91.020101
Abstract
The Floquet eigenvalue problem is analyzed for periodically driven Friedrichs models on discrete and continuous space. In the high-frequency regime, there exists a Floquet bound state consistent with the Floquet-Magnus expansion in the discrete Friedrichs model, while it is not the case in the continuous model. In the latter case, however, the bound state predicted by the Floquet-Magnus expansion appears as a metastable state whose lifetime diverges in the limit of large frequencies. We obtain the lifetime by evaluating the imaginary part of the quasi-energy of the Floquet resonant state. In the low-frequency regime, there is no Floquet bound state and instead the Floquet resonant state with exponentially small imaginary part of the quasi-energy appears, which is understood as the quantum tunneling in the energy space.
5 pages, 3 figures
References in corpus (6)
- Photovoltaic Hall effect in graphene
- The Magnus expansion and some of its applications
- Driven quantum transport on the nanoscale
- Equilibrium states of generic quantum systems subject to periodic driving
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Cited by in corpus (7)
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- Dynamics of fluctuation correlation in periodically driven classical system
- Long time asymptotic state of periodically driven open quantum systems
- Resonances in a periodically driven bosonic system
- Periodically-driven Kondo impurity in nonequilibrium steady states
- Quasiperiodic Floquet-Gibbs states in Rydberg atomic systems
- Statistical prethermalization in randomly kicked many-body classical rotor system