Abstract
Each parameter in a driven Jaynes–Cummings (JC) model of a cavity system is specified in terms of experimental parameters, such as the transmission coefficient of the mirrors, the length of the cavity, and the intensity of the input coherent field. For this purpose, linear and the third-order nonlinear spectra are calculated from the driven JC model, and the results are compared with those from the universe-mode approach which enables us to treat experimental parameters in a straightforward manner. Although the relationships of the parameters are obtained in the high-Q cavity regime, they are also applicable in the low-Q cavity regime.
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