Controllable optical response in hybrid opto-electromechanical systems*
Jiang Chenga)†, Cui Yuan-Shuna), Liu Hong-Xianga),b), Li Xiao-Weia), Chen Gui-Bina)
       
Probe transmission | t |2 as a function of the probe-cavity detuning Δ p = Ω p− ω o when Δ o = ω m and Δ e = − ω m for P e = 0,20,40,60 nW, respectively. The inset shows the peak transmission as a function of the microwave pump power P e when the probe field is resonant with the optical cavity. The optical pump power P o equals 5 μW. Other parameters are the same as those of Fig.  2 .