• Acta Physica Sinica
  • Vol. 68, Issue 3, 034204-1 (2019)
Juan Li, Jia-Ming Li, Chun-Xiao Cai, Heng-Xin Sun, Kui Liu*, and Jiang-Rui Gao
DOI: 10.7498/aps.68.20181625 Cite this Article
Juan Li, Jia-Ming Li, Chun-Xiao Cai, Heng-Xin Sun, Kui Liu, Jiang-Rui Gao. Enhancement of continuous-variable hyperentanglement by optimizing pump mode[J]. Acta Physica Sinica, 2019, 68(3): 034204-1 Copy Citation Text show less
Theoretical inseparability against normalized pump power for three pump modes, (green solid line), (red solid line) and the optimal pump mode (blue solid line) under ideal conditions. The parameters are , .抽运模式分别为模(绿色)、模(红色)以及最佳抽运模式模(蓝色)三种情况下, 纠缠不可分度随归一化抽运功率变化的理论曲线(所取参数为, )
Fig. 1. Theoretical inseparability against normalized pump power for three pump modes, (green solid line), (red solid line) and the optimal pump mode (blue solid line) under ideal conditions. The parameters are , . 抽运模式分别为 模(绿色)、 模(红色)以及最佳抽运模式 模(蓝色)三种情况下, 纠缠不可分度随归一化抽运功率 变化的理论曲线(所取参数为 , )
Experimental setup. RC, three-mirror ring cavity; DBS, dichroic beamsplitter; HWP, half wave plate; PBS, polarizing beamsplitter; PZT, piezoelectric transducer; DP, Dove Prism; MC, mode converter; FQ-PM, four-quadrant phase mask; KTP, KTiOPO4 crystal; MC, mode converter; SA, spectrum analyzer; BHD, balanced homodyne detector.实验装置图, 其中, RC, 三镜环形腔; DBS, 双色分束器; HWP, 半波片; PBS, 偏振分束器; PZT, 压电陶瓷; DP, 道威棱镜; MC, 模式转换器; FQ-PM, 四象限相位片; KTP, KTiOPO4晶体; MC, 模式转换器; SA, 频谱分析仪; BHD, 平衡零拍测量装置
Fig. 2. Experimental setup. RC, three-mirror ring cavity; DBS, dichroic beamsplitter; HWP, half wave plate; PBS, polarizing beamsplitter; PZT, piezoelectric transducer; DP, Dove Prism; MC, mode converter; FQ-PM, four-quadrant phase mask; KTP, KTiOPO4 crystal; MC, mode converter; SA, spectrum analyzer; BHD, balanced homodyne detector. 实验装置图, 其中, RC, 三镜环形腔; DBS, 双色分束器; HWP, 半波片; PBS, 偏振分束器; PZT, 压电陶瓷; DP, 道威棱镜; MC, 模式转换器; FQ-PM, 四象限相位片; KTP, KTiOPO4晶体; MC, 模式转换器; SA, 频谱分析仪; BHD, 平衡零拍测量装置
Measured quantum correlations using the mode: (a1) Amplitude correlation noise of modes; (a2) phase correlation noise of modes; (b1) amplitude correlation noise of modes; (b2) phase correlation noise of modes. (a1) and (b1) Trace1 (red line), ; Trace3 (blue line), . (a2) and (b2) Trace1 (red line), ; Trace3 (blue line), . Trace2 (black line), SNL.模做抽运场的纠缠测量结果 (a1) 模的振幅关联噪声谱; (a2) 模的相位关联噪声谱; (b1) 模的振幅关联噪声谱; (b2) 模的相位关联噪声谱; 黑线(2), SNL; 图(a1)和(b1)中, 红线(1), ; 蓝线(3), ; 图(a2)和(b2)中, 红线(1), ; 蓝线(3),
Fig. 3. Measured quantum correlations using the mode: (a1) Amplitude correlation noise of modes; (a2) phase correlation noise of modes; (b1) amplitude correlation noise of modes; (b2) phase correlation noise of modes. (a1) and (b1) Trace1 (red line), ; Trace3 (blue line), . (a2) and (b2) Trace1 (red line), ; Trace3 (blue line), . Trace2 (black line), SNL. 模做抽运场的纠缠测量结果 (a1) 模的振幅关联噪声谱; (a2) 模的相位关联噪声谱; (b1) 模的振幅关联噪声谱; (b2) 模的相位关联噪声谱; 黑线(2), SNL; 图(a1)和(b1)中, 红线(1), ; 蓝线(3), ; 图(a2)和(b2)中, 红线(1), ; 蓝线(3),
Measured quantum correlations with pumping : (a1) Amplitude correlation noise of modes; (a2) phase correlation noise of modes; (b1) amplitude correlation noise of modes; (b2) phase correlation noise of modes. (a1) and (b1) Trace1 (red line), ; Trace3 (blue line), . (a2) and (b2) Trace1 (red line), ; Trace3 (blue line), . Trace2 (black line), SNL.模做抽运场纠缠测量结果 (a1) 模的振幅关联噪声谱; (a2) 模的相位关联噪声谱; (b1) 模的振幅关联噪声谱; (b2) 模的相位关联噪声谱; 黑线(2), SNL; 图(a1)和(b1)中, 红线(1), ; 蓝线(3), ; 图(a2)和(b2)中, 红线(1), ; 蓝线(3),
Fig. 4. Measured quantum correlations with pumping : (a1) Amplitude correlation noise of modes; (a2) phase correlation noise of modes; (b1) amplitude correlation noise of modes; (b2) phase correlation noise of modes. (a1) and (b1) Trace1 (red line), ; Trace3 (blue line), . (a2) and (b2) Trace1 (red line), ; Trace3 (blue line), . Trace2 (black line), SNL. 模做抽运场纠缠测量结果 (a1) 模的振幅关联噪声谱; (a2) 模的相位关联噪声谱; (b1) 模的振幅关联噪声谱; (b2) 模的相位关联噪声谱; 黑线(2), SNL; 图(a1)和(b1)中, 红线(1), ; 蓝线(3), ; 图(a2)和(b2)中, 红线(1), ; 蓝线(3),
Experimental measurement of inseparability for the orbital angular momentum and spin angular momentum with different pump mode: (a) Orbital angular momentum; (b) spin angular momentum. Blue line (1) and red line (2) respectively represent the results using the mode and mode. Values below 2 indicate entanglement.不同抽运模式下, 轨道角动量纠缠和自旋角动量纠缠的不可分度 (a)轨道角动量纠缠; (b)自旋角动量纠缠; 蓝线(1)和红线(2)分别对应模和模做抽运的结果; 不可分度低于2表示存在纠缠
Fig. 5. Experimental measurement of inseparability for the orbital angular momentum and spin angular momentum with different pump mode: (a) Orbital angular momentum; (b) spin angular momentum. Blue line (1) and red line (2) respectively represent the results using the mode and mode. Values below 2 indicate entanglement. 不同抽运模式下, 轨道角动量纠缠和自旋角动量纠缠的不可分度 (a)轨道角动量纠缠; (b)自旋角动量纠缠; 蓝线(1)和红线(2)分别对应 模和 模做抽运的结果; 不可分度低于2表示存在纠缠
抽运模式
${\rm{LG}}_0^0$${\rm{LG}}_1^0$${\rm{LG}}_2^0$${1 / 3}{\rm{LG}}_0^0 + {2 / 3}{\rm{LG}}_1^0$
耦合系数 ${\varGamma _{{\rm{0}}p}}$${1 / 2}$${1 / {\sqrt 2 }}$00${{\sqrt 3 } / 2}$
Table 1. Coupling coefficient with different pump modes.
Juan Li, Jia-Ming Li, Chun-Xiao Cai, Heng-Xin Sun, Kui Liu, Jiang-Rui Gao. Enhancement of continuous-variable hyperentanglement by optimizing pump mode[J]. Acta Physica Sinica, 2019, 68(3): 034204-1
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