• Acta Physica Sinica
  • Vol. 69, Issue 1, 014207-1 (2020)
Guan-Hua Zuo1, Chen Yang1, Jun-Xiang Zhao1, Zhuang-Zhuang Tian1, Shi-Yao Zhu3, Yu-Chi Zhang2、*, and Tian-Cai Zhang1、*
Author Affiliations
  • 1Collaborative Innovation Center of Extreme Optics, State Key Laboratory of Quantum Qptics and Quantum Optics Devices, Institute of Opto-Electronics, Shanxi University, Taiyuan 030006, China
  • 2College of Physics and Electronic Engineering, Shanxi University, Taiyuan 030006, China
  • 3Department of Physics, Zhejiang University, Hangzhou 310027, China
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    DOI: 10.7498/aps.69.20191009 Cite this Article
    Guan-Hua Zuo, Chen Yang, Jun-Xiang Zhao, Zhuang-Zhuang Tian, Shi-Yao Zhu, Yu-Chi Zhang, Tian-Cai Zhang. Generation of bright polarization squeezed light at cesium D2 line based on optical parameter amplifier [J]. Acta Physica Sinica, 2020, 69(1): 014207-1 Copy Citation Text show less
    Diagrammatic illustration of the quantum Poincaré sphere and Stokes parameters.量子化的庞加莱球和斯托克斯参量图示
    Fig. 1. Diagrammatic illustration of the quantum Poincaré sphere and Stokes parameters.量子化的庞加莱球和斯托克斯参量图示
    Apparatus required to measure four Stokes parameters. PBS, polarizing beam splitter; and , half-and quarter-wave plates, respectively; the plus and minus signs imply that an electrical sum or difference has been taken; SA, Spectrum analyzer.四个斯托克斯参量的测量装置. PBS, 偏振分束棱镜; 和分别是半波片和四分之波片; 加号和减号分别代表电流信号相加减; SA, 频谱分析仪
    Fig. 2. Apparatus required to measure four Stokes parameters. PBS, polarizing beam splitter; and , half-and quarter-wave plates, respectively; the plus and minus signs imply that an electrical sum or difference has been taken; SA, Spectrum analyzer. 四个斯托克斯参量的测量装置. PBS, 偏振分束棱镜; 和 分别是半波片和四分之波片; 加号和减号分别代表电流信号相加减; SA, 频谱分析仪
    Apparatus used to produce the bright polarizationsqueezed beam.明亮偏振压缩光合成装置
    Fig. 3. Apparatus used to produce the bright polarizationsqueezed beam.明亮偏振压缩光合成装置
    Schematic of experimental setup.实验装置图
    Fig. 4. Schematic of experimental setup.实验装置图
    Parametric gain versus pump power, where green (red) solid dots denote the experimental results of amplified (deamplified) gain. The solid lines represent the theoretical results.参量增益随泵浦光功率的变化, 其中绿(红)色实点是参量放大(缩小)的实验结果. 实线是理论拟合结果
    Fig. 5. Parametric gain versus pump power, where green (red) solid dots denote the experimental results of amplified (deamplified) gain. The solid lines represent the theoretical results.参量增益随泵浦光功率的变化, 其中绿(红)色实点是参量放大(缩小)的实验结果. 实线是理论拟合结果
    Noise power when scanning the local beam phase. The spectrum analyzer’s center frequency is 2 MHz with RBW = 100 kHz and VBW = 500 Hz.扫描本地光相位时得到的噪声. 谱仪中心频率为2 MHz, 分辨率带宽(RBW)为100 kHz, 视频带宽(VBW)为500 Hz
    Fig. 6. Noise power when scanning the local beam phase. The spectrum analyzer’s center frequency is 2 MHz with RBW = 100 kHz and VBW = 500 Hz. 扫描本地光相位时得到的噪声. 谱仪中心频率为2 MHz, 分辨率带宽(RBW)为100 kHz, 视频带宽(VBW)为500 Hz
    Measured noise results for different Stokes parameters. The results on the left are the measured variance spectra of Stokes parameters normalized to quantum noise limit. The results on the right are the corresponding diagrammatic illustration of the Stokes parameters’ variance ellipsoid, and the blue ellipsoid is the noise ball, and these ellipses are the noise projections at each plane. The red dashed circles represent the noise of the coherent state and the blue solid circles show the squeezing. (a) Squeezing for Stokes parameter ; (b) Squeezing for Stokes parameter ; (c) Squeezing for Stokes parameter .不同斯托克斯参量的噪声测量结果. 其中左图是测量的斯托克斯参量的噪声谱, 已归一化到标准量子噪声基准. 右图是与之对应的噪声分布球及投影噪声分布, 其中蓝色椭球体代表噪声球, 椭圆表示噪声球投影到各个面上的噪声分布. 红色虚线表示相干光对应的噪声, 蓝色实线表示偏振压缩光 (a) 压缩; (b) 压缩; (c) 压缩
    Fig. 7. Measured noise results for different Stokes parameters. The results on the left are the measured variance spectra of Stokes parameters normalized to quantum noise limit. The results on the right are the corresponding diagrammatic illustration of the Stokes parameters’ variance ellipsoid, and the blue ellipsoid is the noise ball, and these ellipses are the noise projections at each plane. The red dashed circles represent the noise of the coherent state and the blue solid circles show the squeezing. (a) Squeezing for Stokes parameter ; (b) Squeezing for Stokes parameter ; (c) Squeezing for Stokes parameter . 不同斯托克斯参量的噪声测量结果. 其中左图是测量的斯托克斯参量的噪声谱, 已归一化到标准量子噪声基准. 右图是与之对应的噪声分布球及投影噪声分布, 其中蓝色椭球体代表噪声球, 椭圆表示噪声球投影到各个面上的噪声分布. 红色虚线表示相干光对应的噪声, 蓝色实线表示偏振压缩光 (a) 压缩; (b) 压缩; (c) 压缩
    参数
    传输效率0.99
    量子效率0.95
    干涉效率0.986
    逃逸率0.73
    归一化泵浦因子0.71
    归一化测量频率0.18
    Table 1. Factors of effecting squeezing from the OPA and the detection system.
    Guan-Hua Zuo, Chen Yang, Jun-Xiang Zhao, Zhuang-Zhuang Tian, Shi-Yao Zhu, Yu-Chi Zhang, Tian-Cai Zhang. Generation of bright polarization squeezed light at cesium D2 line based on optical parameter amplifier [J]. Acta Physica Sinica, 2020, 69(1): 014207-1
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