• Infrared and Laser Engineering
  • Vol. 49, Issue 8, 2020018 (2020)
Heng Wei1, Lin Lu2, Tao Pu2, Jilin Zheng2..., Jiyong Zhao2, Baofu Zhang2 and Chuanxin Wu2|Show fewer author(s)
Author Affiliations
  • 1College of Communication Engineering, Army Engineering University of PLA, Nanjing 210007, China
  • 2College of Communication Engineering, Army Engineering University of PLA, Nanjing 210007, China
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    DOI: 10.3788/IRLA20200018 Cite this Article
    Heng Wei, Lin Lu, Tao Pu, Jilin Zheng, Jiyong Zhao, Baofu Zhang, Chuanxin Wu. Fiber time delay fluctuations measurement based on one-way transfer[J]. Infrared and Laser Engineering, 2020, 49(8): 2020018 Copy Citation Text show less

    Abstract

    In order to be compatible with the existing optical communication network, a time delay fluctuations measurement based on "single-fiber one-way" transfer scheme was proposed. Based on the temperature-induced variation of group velocity dispersion effect and Sellmeier equation, a proportionality model for calculating the one-way delay fluctuations was established with detecting the delay difference fluctuations between two propagating optical signals at given different wavelengths and accurate temperature measurement. Assuming proportionality coefficient in the model was the ratio between one-way delay fluctuations and one-way dual wavelength delay difference fluctuations. By simulation, the impact of fiber link parameters, such as temperature and wavelength difference, on proportionality coefficient was discussed. The experimental platform for one-way time transfer over 75 km fiber was conducted and the experimental results show that the measured proportional coefficient is -258.4, close to the theoretical proportional coefficient -277.3, and the corresponding one-way delay variation error is 660 ps. The measured results validate the correctness of the proposed model as well as the possibility of fiber time delay fluctuations measurement based on one-way transfer.
    $\tau = \frac{L}{c}\left( {n - \lambda \frac{{{\rm d}n}}{{{\rm d}\lambda }}} \right)$(1)

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    $dτdT|λN=1c[dLdT(nλNλNdnλNdλN)+L(dnλNdTλNd2nλNdλNdT)],N=1,2 $(2)

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    $dτdT|λ1λ2=1c[dLdT((nλ1nλ2)+λ2dnλ2dλ2λ1dnλ1dλ1)+L(ddT((nλ1nλ2)+λ2dnλ2dλ2λ1dnλ1dλ1))] $(3)

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    $M=dτdT|λ1dτdT|λ1λ2=Lc(dnλ1dTλ1d2nλ1dλ1dT)Lc(dnλ1dTdnλ2dT+λ2d2nλ2dλ2dTλ1d2nλ1dλ1dT)=dnλ1dTλ1d2nλ1dλ1dTdnλ1dTdnλ2dT+λ2d2nλ2dλ2dTλ1d2nλ1dλ1dT $(4)

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    ${n^2}\left( {\lambda ,T} \right) - 1 = \sum\limits_{i = 1}^3 {\frac{{{S_i}\left( T \right){\lambda ^2}}}{{{\lambda ^2} - \lambda _i^2\left( T \right)}}} $(5)

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    ${\text{单波长时延波动}} = {\text{测得双波长时延差波动}}*M$(6)

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    Heng Wei, Lin Lu, Tao Pu, Jilin Zheng, Jiyong Zhao, Baofu Zhang, Chuanxin Wu. Fiber time delay fluctuations measurement based on one-way transfer[J]. Infrared and Laser Engineering, 2020, 49(8): 2020018
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