• Photonics Research
  • Vol. 9, Issue 2, 222 (2021)
Xiao Li1、2、†, Meizhen Ren3、†, Jiashun Zhang1, Liangliang Wang1, Wei Chen4, Yue Wang1, Xiaojie Yin1, Yuanda Wu1、2, and Junming An1、2、*
Author Affiliations
  • 1State Key Laboratory on Integrated Optoelectronics, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Division of Quantum Materials and Devices, Beijing Academy of Quantum Information Sciences, Beijing 100193, China
  • 4Laboratory of Quantum Information, CAS, University of Science and Technology of China, Hefei 230026, China
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    DOI: 10.1364/PRJ.406123 Cite this Article Set citation alerts
    Xiao Li, Meizhen Ren, Jiashun Zhang, Liangliang Wang, Wei Chen, Yue Wang, Xiaojie Yin, Yuanda Wu, Junming An. Interference at the single-photon level based on silica photonics robust against channel disturbance[J]. Photonics Research, 2021, 9(2): 222 Copy Citation Text show less
    Silica PLC device. (a) Schematic of our AMZI chip. (b) A photograph of the chip packaging. The device contacts the surface of the TEC platform and is covered with a heat-insulating shell when the operation is on.
    Fig. 1. Silica PLC device. (a) Schematic of our AMZI chip. (b) A photograph of the chip packaging. The device contacts the surface of the TEC platform and is covered with a heat-insulating shell when the operation is on.
    (a) Experimental setup to investigate the polarization characteristics of a 740 ps delay AMZI chip at the single-photon level. Att., variable optical attenuator; DC, direct current voltage drive; TEC, temperature controller. (b) Graph illustrating the pulse self-interfering method.
    Fig. 2. (a) Experimental setup to investigate the polarization characteristics of a 740 ps delay AMZI chip at the single-photon level. Att., variable optical attenuator; DC, direct current voltage drive; TEC, temperature controller. (b) Graph illustrating the pulse self-interfering method.
    (a) Interference fringes observed for 740 ps delay AMZI chip when device temperature is scanned from 10°C to 60°C. (b) The fitting curve of our proposed model by Eq. (8). The y axis represents normalized amplitude, y=(5.46×T+13)×(0.089×T−1.29), where V=0 (volt).
    Fig. 3. (a) Interference fringes observed for 740 ps delay AMZI chip when device temperature is scanned from 10°C to 60°C. (b) The fitting curve of our proposed model by Eq. (8). The y axis represents normalized amplitude, y=(5.46×T+13)×(0.089×T1.29), where V=0 (volt).
    Experimental setup with minor variation on the one in Fig. 2(a). PBS, polarization beam splitter. Single-mode fiber (SMF) is in yellow; polarization maintaining fiber (PMF) is in blue.
    Fig. 4. Experimental setup with minor variation on the one in Fig. 2(a). PBS, polarization beam splitter. Single-mode fiber (SMF) is in yellow; polarization maintaining fiber (PMF) is in blue.
    (a) Interference fringes versus device temperature, associated with the TE (red) and TM (blue) modes. The top black curve is the sum of the TE and TM modes. The minimum visibility occurs at 29.2°C, corresponding to Δϕ=(2N+1)π, while the maximum visibility occurs at 49°C, corresponding to Δϕ=2Nπ. (b) and (c) Interference fringes of the TE (red) and TM (blue) modes versus voltage square of TOPM2 at 29.2°C and 49°C, respectively. The fringes of both modes are in anti-phase at 29.2°C and in phase at 49°C, which agrees with the phase matching shown in (a).
    Fig. 5. (a) Interference fringes versus device temperature, associated with the TE (red) and TM (blue) modes. The top black curve is the sum of the TE and TM modes. The minimum visibility occurs at 29.2°C, corresponding to Δϕ=(2N+1)π, while the maximum visibility occurs at 49°C, corresponding to Δϕ=2Nπ. (b) and (c) Interference fringes of the TE (red) and TM (blue) modes versus voltage square of TOPM2 at 29.2°C and 49°C, respectively. The fringes of both modes are in anti-phase at 29.2°C and in phase at 49°C, which agrees with the phase matching shown in (a).
    Interference fringes of the TE (red) and TM (blue) modes versus device temperature scanned from 10°C to 50°C; (a) and (b) correspond to 200 ps and 400 ps, respectively. The top black curve is the sum of the TE and TM modes.
    Fig. 6. Interference fringes of the TE (red) and TM (blue) modes versus device temperature scanned from 10°C to 50°C; (a) and (b) correspond to 200 ps and 400 ps, respectively. The top black curve is the sum of the TE and TM modes.
    Interference fringes of the TE (red) and TM (blue) modes versus device temperature, scanned from 10°C to 60°C for Bob’s 740 ps delay AMZI chip. The top black curve is the sum of the TE and TM modes.
    Fig. 7. Interference fringes of the TE (red) and TM (blue) modes versus device temperature, scanned from 10°C to 60°C for Bob’s 740 ps delay AMZI chip. The top black curve is the sum of the TE and TM modes.
    Experimental setup to prove robustness against polarization disturbance of our interferometers based on silica 740 ps delay AMZI chips.
    Fig. 8. Experimental setup to prove robustness against polarization disturbance of our interferometers based on silica 740 ps delay AMZI chips.
    Fringe visibility versus T ranging from 34°C to 39.6°C. The inset shows interference fringes over 20 km transmission, at the optimal T of 36.6°C.
    Fig. 9. Fringe visibility versus T ranging from 34°C to 39.6°C. The inset shows interference fringes over 20 km transmission, at the optimal T of 36.6°C.
    Proof of long-term stability of our setup. Plot of the extinction ratio between the two outputs from Bob against time over 6 h. The inset shows interference fringes of the two outputs of Bob’s AMZI chip.
    Fig. 10. Proof of long-term stability of our setup. Plot of the extinction ratio between the two outputs from Bob against time over 6 h. The inset shows interference fringes of the two outputs of Bob’s AMZI chip.
    Xiao Li, Meizhen Ren, Jiashun Zhang, Liangliang Wang, Wei Chen, Yue Wang, Xiaojie Yin, Yuanda Wu, Junming An. Interference at the single-photon level based on silica photonics robust against channel disturbance[J]. Photonics Research, 2021, 9(2): 222
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