• Photonics Research
  • Vol. 9, Issue 11, 2176 (2021)
Guo-Wei Zhang1、2, Yu-Yang Ding3、6、*, Wei Chen1、2、7、*, Fang-Xiang Wang1、2, Peng Ye1、2, Guan-Zhong Huang1、2, Shuang Wang1、2, Zhen-Qiang Yin1、2, Jun-Ming An4、5, Guang-Can Guo1、2, and Zheng-Fu Han1、2
Author Affiliations
  • 1CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China
  • 2CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei 230026, China
  • 3Hefei Guizhen Chip Technologies Co., Ltd., Hefei 230000, China
  • 4State Key Laboratory on Integrated Optoelectronics, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 5Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 6e-mail: dingyuyang@gz-ichip.com
  • 7e-mail: weich@ustc.edu.cn
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    DOI: 10.1364/PRJ.432327 Cite this Article Set citation alerts
    Guo-Wei Zhang, Yu-Yang Ding, Wei Chen, Fang-Xiang Wang, Peng Ye, Guan-Zhong Huang, Shuang Wang, Zhen-Qiang Yin, Jun-Ming An, Guang-Can Guo, Zheng-Fu Han. Polarization-insensitive interferometer based on a hybrid integrated planar light-wave circuit[J]. Photonics Research, 2021, 9(11): 2176 Copy Citation Text show less
    AFMI device. (a) Scheme of our AFMI. The interferometer combines an FA for photon coupling, a DC with the splitting ratio of 50:50, a 200 ps delay line, and two FMs; (b) photograph of our AFMI. The size of the chip is about 27.8 mm×23.1 mm, and the length of the FM is about 17.5 mm. A copper heat sink with a TEC and a thermistor is attached to the back of the chip. The entire system is packaged in an aluminum box with temperature isolation (not shown in this figure).
    Fig. 1. AFMI device. (a) Scheme of our AFMI. The interferometer combines an FA for photon coupling, a DC with the splitting ratio of 50:50, a 200 ps delay line, and two FMs; (b) photograph of our AFMI. The size of the chip is about 27.8  mm×23.1  mm, and the length of the FM is about 17.5 mm. A copper heat sink with a TEC and a thermistor is attached to the back of the chip. The entire system is packaged in an aluminum box with temperature isolation (not shown in this figure).
    Experimental setup to evaluate the characteristics of our AFMIs. Laser, gain-switch laser source; TEC, temperature controller; ATT, light attenuator; PC, polarization controller; Cir, circulator; SPD1 and SPD2, single-photon detectors.
    Fig. 2. Experimental setup to evaluate the characteristics of our AFMIs. Laser, gain-switch laser source; TEC, temperature controller; ATT, light attenuator; PC, polarization controller; Cir, circulator; SPD1 and SPD2, single-photon detectors.
    Interference results with temperature scanning of AFMI1. The black dots are measured data points, and the red line is the corresponding curve fitting.
    Fig. 3. Interference results with temperature scanning of AFMI1. The black dots are measured data points, and the red line is the corresponding curve fitting.
    Interference results for fixed polarization states.
    Fig. 4. Interference results for fixed polarization states.
    Results of continuous polarization scramble test. (a) Diagram of interference visibility with and without continuous polarization scramble; insets, the diagram of normalized Stokes parameters and interference visibility during test; (b) visibilities in the range of 10°C–35°C with and without polarization scramble. The 3σ error bar is selected as the confidence interval using 10 min testing data.
    Fig. 5. Results of continuous polarization scramble test. (a) Diagram of interference visibility with and without continuous polarization scramble; insets, the diagram of normalized Stokes parameters and interference visibility during test; (b) visibilities in the range of 10°C–35°C with and without polarization scramble. The 3σ error bar is selected as the confidence interval using 10 min testing data.
    Results of long-term phase stability test. Shadow areas represent the 1σ error bar.
    Fig. 6. Results of long-term phase stability test. Shadow areas represent the 1σ error bar.
    Results of delay difference calculation. (a) Variations of the visibilities for temporal and amplitude mismatch. The red triangle is where our AFMIs stand. (b) Normalized light intensity after propagating through two AFMIs, detected by an SPD. The ΔT represents relative delay time.
    Fig. 7. Results of delay difference calculation. (a) Variations of the visibilities for temporal and amplitude mismatch. The red triangle is where our AFMIs stand. (b) Normalized light intensity after propagating through two AFMIs, detected by an SPD. The ΔT represents relative delay time.
    Guo-Wei Zhang, Yu-Yang Ding, Wei Chen, Fang-Xiang Wang, Peng Ye, Guan-Zhong Huang, Shuang Wang, Zhen-Qiang Yin, Jun-Ming An, Guang-Can Guo, Zheng-Fu Han. Polarization-insensitive interferometer based on a hybrid integrated planar light-wave circuit[J]. Photonics Research, 2021, 9(11): 2176
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