Fig. 1. Schematic diagram of the system ^[25]. 系统原理图^[25]

Fig. 2. The relationship between the transmissivity and the frequency detuning of the probe light and the cavity mode ( ) at different pump power. The frequency of the pump light satisfies the condition of blue detuning( ). 透射率 在不同的抽运光功率下, 随探测光与腔模的频率失谐量 的变化, 抽运光的频率满足蓝失谐条件

Fig. 3. When the input probe light is squeeze light, the squeeze component of the linear part of the output light varies with the effective detection-cavity detuning value ( ). The squeeze angle of the probe light is (a) 0, (b) π/4, (c) π/2 (d) 3π/4 在输入的探测光为压缩光的情况下, 输出光的线性部分的压缩分量 随有效探测-腔失谐量 的变化, 探测压缩光的压缩角θ为(a) 0, (b) π/4, (c) π/2 (d) 3π/4

Fig. 4. The variation of the squeeze parameter S₁ of the linear part of the output light with the squeeze amplitude r of the incident probe light, the squeeze angle of the incident probe light is θ = 0, and the frequency is resonant with the cavity mode . 输出光的线性部分的压缩量 随入射探测光的压缩幅r的变化, 入射探测光的压缩角为θ = 0, 频率与腔模共振

Fig. 5. The squeeze parameter S₁ of the non-linear part of the output light varies with the frequency of the incident probe squeeze light in the case of different squeeze amplitudes of the incident squeeze light, is the frequency detuning between the probe light and the cavity mode. 在不同入射压缩光压缩幅的情况下, 输出光中的非线性部分的压缩量 随入射探测压缩光频率的变化. 为探测光与腔模的频率失谐