Floquet-state cooling
arXiv:1911.12563 · doi:10.1038/s41598-019-53877-w
Abstract
We demonstrate that a periodically driven quantum system can adopt a quasistationary state which is effectively much colder than a thermal reservoir it is coupled to, in the sense that certain Floquet states of the driven-dissipative system can carry much higher population than the ground state of the corresponding undriven system in thermal equilibrium. This is made possible by a rich Fourier spectrum of the system's Floquet transition matrix elements, the components of which are addressed individually by a suitably peaked reservoir density of states. The effect is expected to be important for driven solid-state systems interacting with a phonon bath predominantly at well-defined frequencies.
15 pages, 3 figures
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- Binary Bose-Einstein condensates in a disordered time-dependent potential
- Defining a well-ordered Floquet basis by the average energy
- Periodic thermodynamics of a two spin Rabi model
- Dissipative preparation of a Floquet topological insulator in an optical lattice via bath engineering
- Environment-controlled Floquet-state paramagnetism