Figure 12
Correlation functions \(\log {g_{i}^{(2)}(0)}\) versus the frequency detuning \(\Delta _{_\mathrm{SMR}}\) in units of \(\gamma\) for the QD-driven system for the resonant case with \(\omega _{_\mathrm{SMR}}=\omega _{m}=\omega _q=\gamma \times 1560\) MHz (so also \(\Delta _a=\Delta _b=\Delta _q\)). The thin curves in each mode are obtained using the master equation in Eq. (12) and the thick curves are obtained from the non-Hermitian Hamiltonian method using Eqs. (22) and (23). Parameters are set in Eq. (29) except \(g=4.5\gamma\) and \(\kappa _a=\kappa _b=6\gamma\).
