• 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

    Abstract

    Quantum key distribution (QKD) provides a solution for communication of unconditional security. However, the quantum channel disturbance in the field severely increases the quantum bit-error rate, degrading the performance of a QKD system. Here we present a setup comprising silica planar light wave circuits (PLCs), which is robust against the channel polarization disturbance. Our PLCs are based on the asymmetric Mach–Zehnder interferometer (AMZI), integrated with a tunable power splitter and thermo-optic phase modulators. The polarization characteristics of the AMZI PLC are investigated by a novel pulse self-interfering method to determine the operation temperature of implementing polarization insensitivity. Over a 20 km fiber channel with 30 Hz polarization scrambling, our time-bin phase-encoding QKD setup is characterized with an interference fringe visibility of 98.72%. The extinction ratio for the phase states is kept between 18 and 21 dB for 6 h without active phase correction.
    N=NsTE+NlTE+2NsTENlTEcos(ΔϕTE)+NsTM+NlTM+2NsTMNlTMcos(ΔϕTM),

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    ΔϕTE=2πλ0nTE(T)ΔL+ϕ(V2),

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    ΔϕTM=2πλ0nTM(T)ΔL+ϕ(V2).

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    Δϕ=ΔϕTEΔϕTM=2πΔnΔLλ0,

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    NsTE=NlTE=N12,

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    NsTM=NlTM=N22.

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    ΔϕTE=ΔϕTM+Δϕ.

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    N=N1+N2+2N1N2cos(ΔϕTM+Δϕ2)cos(Δϕ2)=N1+N2+2N1N2cos(a2πλ0ΔL·T+b·V2+c)cos(d·T+e),

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    V=NmaxNminNmax+Nmin=2N1N2N1+N2·|cosΔϕ2|=2N1N2N1+N2·|cos(d·T+e)|.

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    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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