Triple optomechanical induced transparency in a two-cavity system

Wu Shi-Chao^{1, 2}, Qin Li-Guo^{2, †,}, Jing Jun³, Yang Guo-Hong¹, Wang Zhong-Yang^{2, ‡,}

(a) The absorption Re[ɛ_T] and (b) dispersion Im[ɛ_T] as a function of (δ − ω_b)/ω_b without the optomechanical coupling, i.e, g_a = g_c = 0. (c) The absorption Re[ɛ_T] and (d) dispersion Im[ɛ_T] as a function of δ/ω_b with the coupling between cavity c and optomechanical resonator d being zero, i.e., g_c = 0. The other parameters are the same as those in Fig. 2.