Fig. presents the results of absorption of the same toluene-cavity hybrid system. In particular, the work in Ref. 193 uses scQED simulations to directly examine the condition to achieve a strong coupling by incorporating cavity loss into the analysis. This is done through broadening of the cavity coupling strength across a multitude of cavity modes localized at the primary cavity frequency ω c following a Lorentzian broadening of varied width κ (i.e., loss rate). The coupling strength λ (Eq. 105) is distributed across the multitude of modes in the spectral function (i.e., a Lorentzian) such that