The authors derive an exact propagator for the open dispersive Jaynes-Cummings model and a second-order perturbative solution for the open quantum Rabi model, revealing a non-thermal qubit steady state that is unique to the Rabi model.
In the Bargmann space the coherent state can be written as FB (ρα;z,z∗) =e−|α|2+zα+z∗α ∗
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Analytical solution of the open dispersive Jaynes-Cummings model and perturbative analytical solution of the open quantum Rabi model
The authors derive an exact propagator for the open dispersive Jaynes-Cummings model and a second-order perturbative solution for the open quantum Rabi model, revealing a non-thermal qubit steady state that is unique to the Rabi model.