Figure 8
Correlation functions \(\log {g_{i}^{(2)}(0)}\) versus the frequency detuning \(\Delta _{_\mathrm{SMR}}\) (in units of the qubit decay rate \(\gamma\)) between the drive and SMR for: (a) the resonance case \(\omega _{_\mathrm{SMR}}= \omega _{m}=\omega _q\) (so also \(\Delta _{_\mathrm{SMR}} =\Delta _{m}=\Delta _q\)) and (b) the nonresonance case \(\omega _{_\mathrm{SMR}}\ne \omega _{m}\ne \omega _q\), where \(\omega _b/\gamma =1560\) MHz. Note that by changing the pump frequency, different detunings appear with respect to the modes a and b, and qubit. We set \(g=7.5\gamma\) and other parameters are given in Eq. (28). The numbering of the coloured regions correspond to the cases listed in Table 1.
