Floquet systems coupled to particle reservoirs
arXiv:1412.5599 · doi:10.1103/PhysRevB.91.184301
Abstract
Open quantum systems, when driven by a periodic field, can relax to effective statistical ensembles that resemble their equilibrium counterparts. We consider a class of problems in which a periodically- driven quantum system is allowed to exchange both energy and particles with a thermal reservoir. We demonstrate that, even for noninteracting systems, effective equilibration to the grand canonical ensemble requires both fine tuning the system-bath coupling and selecting a sufficiently simple driving protocol. We study a tractable subclass of these problems in which the long-time steady state of the system can be determined analytically, and demonstrate that the system effectively thermalizes with fine tuning, but does not thermalize for general values of the system-bath couplings. When the driven system does not thermalize, it supports a tunable persistent current in the steady state without external bias. We compute this current analytically for two examples of interest: 1) a driven double quantum dot, where the current is interpreted as a DC electrical current, and 2) driven Dirac fermions in graphene, where it is interpreted as a valley current.
15 pages, 6 figures; Revised version includes small changes. Note title change (in response to referees' comments)
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- Quadratic band touching points and flat bands in two-dimensional topological Floquet systems
- Keldysh approach to periodically driven systems with a fermionic bath: non-equilibrium steady state, proximity effect and dissipation
- Long time asymptotic state of periodically driven open quantum systems
- Periodically-driven Kondo impurity in nonequilibrium steady states