Controllable optical response in hybrid opto-electromechanical systems*
Jiang Chenga)†, Cui Yuan-Shuna), Liu Hong-Xianga),b), Li Xiao-Weia), Chen Gui-Bina)
       
Peak probe transmission | t |2 at the cavity resonance as a function of the optical pump power P o when Δ o = − ω m and Δ e = ω m. The microwave pump power P e is equal to 1 μW. Other parameters are the same as those of Fig.  2 .