Acta Optica Sinica, Volume. 44, Issue 1, 0106013(2024)

Coding Technique for Distributed Fiber Sensors

Quancong Lin, Linghao Cheng*, Lü Jie, Tianfang Zhang, Hao Liang**, and Baiou Guan
Author Affiliations
  • Guangdong Key Laboratory of Fiber Sensing and Communication Technology, Institute of Photonics Technology, Jinan University, Guangzhou 510632, Guangdong , China
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    Figures & Tables(14)
    DOFS system based on coding pulse sequence (AWG: arbitrary waveform generator; AMP: amplifier; SOA: semiconductor amplifier; EDFA: erbium-doped fiber amplifier; ICR: integrated coherent receiver; DAQ: data acquisition)
    Principle of Simplex coding technique[16]
    Binary phase shift keying (BPSK) modulation realized through EOM[27]
    AOM working principle and experimental device diagram[31]. (a) Schematic diagram of basic working principle of AOM; (b) experimental setup for testing phase shifted pulsing method based on AOM
    64-element Frank sequence phase, constellation, and aperiodic autocorrelation functions[45]. (a) Phase of 64-element Frank sequence; (b) constellation of 64-element Frank sequence; (c) aperiodic autocorrelation function of 64-element Frank sequence
    MF of some coding sequences with 256 bit[45]
    Constellations of 256-bit Frank sequence and its optimized sequence[45]
    Frank sequence waveform and phase diagram[45]. (a) 200 MHz waveform carrying optimized Frank sequence generated by AWG and after AOM modulation; (b) phases carried by optimized Frank sequence in Fig. 8(a)
    Φ-OTDR experimental setup of WFBG array with polyphase unimodular coding[45]
    Aperiodic autocorrelations of two sequences after 50 km fiber transmission[45]. (a) Optimized Frank sequence with 1024 bit; (b) PRBS sequence with 1023 bit
    • Table 1. Summary of performance of fiber optic Rayleigh sensors based on coding technology

      View table

      Table 1. Summary of performance of fiber optic Rayleigh sensors based on coding technology

      YearAuthorEncoding typePerformanceRef. No
      1993Jones M DSimplex

      Code length:4 bit;

      relative to Golay code or single pulse OTDR,

      noise power is reduced by 1.9 dB

      46
      2005Lee et al.Simplex

      Sensing distance:20 km;

      compared with the traditional OTDR

      coding gain is improved by 9.04 dB

      47
      2006Lee et al.Simplex

      Code length:255 bit;

      SNR:9.2 dB

      16
      2008Sahu et al.CCPONS

      Same measurement time and peak value;

      SNR is improved by 0.1 dB

      48
      2019Zhang et al.Digital linear frequency modulation(LFM)

      Sensing distance:100 km;

      dynamic range is improved by 7 dB;

      spatial resolution is improved by 10 times

      49
      2019Liao et al.Golay

      Sensing distance:23.8 km;

      smpling rate:4000 MHz;

      SNR:3 dB;

      coding gain:20 dB

      50
      2019Wang et al.Golay

      Sensing distance:10 km;

      submeter gauge length and nanostrain resolution

      51
      2019Mompó et al.Biphase Legendre sequence

      Scan rate:107 kHz;

      spatial resolution:10 cm;

      sensitivity:1.1 mrad/Hz

      30
      2021Tomboza et al.Golay

      Detection distance:1 km;

      good tracking ability

      52
      2023Li et al.Random sequence CPP

      Distortion coefficient:9.23%;

      SIR(signal-to-interference ratio):16.67 dB;

      SNR:21.99 dB

      29
    • Table 2. Summary of performance of fiber optic Raman sensors based on coding technology

      View table

      Table 2. Summary of performance of fiber optic Raman sensors based on coding technology

      YearAuthorEncoding typePerformanceRef. No
      2018Wang et al.SimplexBy increasing the code length,the temperature measurement error is reduced while maintaining the same spatial resolution17
      2018Daiet al.RZ Simplex and complementary RZ Simplex

      Sensing distance:56 km;

      spatial resolution:10 m;

      sensing distance:50 km;

      temperature resolution:1.8 ℃

      18
      2020Sunet al.GO-code

      Sensing distance:10.2 km;

      spatial resolution:2 m;

      measurement time:1 s;

      decoding time:1.6 ms

      25
      2023Faralli et al.Cyclic-Simplex and Simplex binary codesAvoid performance degradation due to nonlinear effects and code word distortion19
    • Table 3. Summary of performance of fiber optic Brillouin sensors based on coding technology

      View table

      Table 3. Summary of performance of fiber optic Brillouin sensors based on coding technology

      YearAuthorEncoding typePerformanceRef. No
      2010Soto et al.Coding technique with RZ modulation format

      Sensing distance:25 km;

      spatial resolution:1 m;

      coding gain:7.2 dB

      54
      2016Denisovet al.PRBS

      Sensing distance:17.5 km;

      spatial resolution:8.3 mm

      55
      2017Sun et al.Rre-pumped Golay

      Sensing distance:50 km;

      spatial resolution:70 cm;

      temperature resolution:<1.5 °C

      56
      2017Wang et al.Rre-depletion two-wavelength probe pulse

      Sensing distance:10.164 km;

      spatial resolution:2 m;

      frequency instability of measurement:0.37 MHz

      23
      2018Zan et al.A pair of detection pulses of different durations

      Sensing distance:350 m;

      spatial resolution:0.2 m;

      Brillouin frequency accuracy:3.2 MHz

      57
      2018Li et al.Golay-DPP

      Sensing distance:10.164 km;

      spatial resolution:50 cm;

      frequency uncertainty:1.4 MHz

      58
      2020Zan et al.Golay

      Sensing distance:1280 m;

      spatial resolution:40 cm;

      Brillouin frequency accuracy:3.47 MHz

      59
      2021Zhou et al.Hybrid aperiodic(HA)coding

      Sensing distance:117.46 km;

      SNR:8 dB;

      measurement certainty:1.67 MHz

      60
      2022Li et al.Golay code under oversampling

      Sensing distance:64 km;

      spatial resolution:6 m

      61
      2022Wei et al.Golay

      Sensing distance:9.63 km;

      spatial resolution:0.5 m

      62
      2022Wang et al.Random coding

      Code length:512 bit;

      coding gain:11.93 dB

      21
    • Table 4. Summary of performance of fiber weak grating array sensors based on coding technology

      View table

      Table 4. Summary of performance of fiber weak grating array sensors based on coding technology

      YearAuthorEncoding typePerformanceRef. No
      2018Dorize et al.Two mutually orthogonal complementary Golay sequence pairs

      Number of fiber Bragg gratings:10;

      bandwidth coverage:18 kHz

      71
      2019Fu et al.Interferometric-noise-suppressing Golay

      In the case of similar SNR;

      acquisition time is reduced to 1/8;

      temperature sensitivity linearity:0.9986;

      wavelength demodulation error:±5 pm

      72
      2022Tang et al.Golay

      Sensing distance:1.5 km ultra-weak fiber Bragg grating(UWFBG);

      Compared with the individual pulse system,

      SNR is improved by 4. 6 dB

      73
      2023Zhang et al.PRBS

      Crosstalk rejection ratio:50 dB;

      dynamic range:30 dB

      74
      2023Zhang et al.Polyphase unimodular sequence

      Sensing distance:50 km;

      crosstalk rejection ratio can be enhanced by more than 10 dB over that of PRBS

      45
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    Quancong Lin, Linghao Cheng, Lü Jie, Tianfang Zhang, Hao Liang, Baiou Guan. Coding Technique for Distributed Fiber Sensors[J]. Acta Optica Sinica, 2024, 44(1): 0106013

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    Paper Information

    Category: Fiber Optics and Optical Communications

    Received: Aug. 15, 2023

    Accepted: Sep. 28, 2023

    Published Online: Jan. 12, 2024

    The Author Email: Cheng Linghao (chenglh@ieee.org), Liang Hao (tlianghao@jnu.edu.cn)

    DOI:10.3788/AOS231418

    CSTR:32393.14.AOS231418

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