Controllable optical response in hybrid opto-electromechanical systems<xref ref-type="fn" rid="cpb142177fn1">*</xref>

Controllable optical response in hybrid opto-electromechanical systems*

Jiang Cheng^a)†, Cui Yuan-Shun^a), Liu Hong-Xiang^a),^b), Li Xiao-Wei^a), Chen Gui-Bin^a)

Probe transmission | t |² versus probe-cavity detuning Δ _p = Ω _p− ω _o for P _o = 0, 10, and 40 μW, respectively. Here, the optical cavity is pumped on its blue sideband and the microwave cavity is pumped on its red sideband, i.e., Δ _o = − ω _m and Δ _e = ω _m. The inset of Figs. 2(b) and 2(c) show the probe transmission near the resonant region on an enlarged scale. Other parameters are P _e = 1 μW, ω _o = 2 π × 282 THz, ω _e = 2 π × 7.1 GHz, κ _o = 2 π × 1.65 MHz, κ _e = 2 π × 1.6 MHz, κ _o,ext = 0.76 κ _o, κ _e,ext = 0.11 κ _e, g _o = 2 π × 27 Hz, g _e = 2 π × 2.7 Hz, ω _m = 2 π × 5.6 MHz, and γ _m = 2 π × 4 Hz.