• Laser & Optoelectronics Progress
  • Vol. 58, Issue 13, 1306011 (2021)
Yahui Wang1、2, Le Zhao1, Qian Zhang1、2, Lijun Qiao1, Tao Wang1, Jianzhong Zhang1、2, and Mingjiang Zhang1、2、*
Author Affiliations
  • 1Key Laboratory of Advanced Transducers and Intelligent Control System, Ministry of Education, Taiyuan University of Technology, Taiyuan , Shanxi 030024, China
  • 2College of Physics and Optoelectronics, Taiyuan University of Technology, Taiyuan , Shanxi 030024, China
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    DOI: 10.3788/LOP202158.1306011 Cite this Article Set citation alerts
    Yahui Wang, Le Zhao, Qian Zhang, Lijun Qiao, Tao Wang, Jianzhong Zhang, Mingjiang Zhang. Progress in Chaotic Brillouin Optical Correlation-Domain Analysis[J]. Laser & Optoelectronics Progress, 2021, 58(13): 1306011 Copy Citation Text show less
    Chaotic laser source and its output characteristics. (a) Single feedback loop external cavity chaotic laser source; (b1) optical spectrum; (b2) radio frequency spectrum; (b3) time sequence; (b4) autocorrelation curve
    Fig. 1. Chaotic laser source and its output characteristics. (a) Single feedback loop external cavity chaotic laser source; (b1) optical spectrum; (b2) radio frequency spectrum; (b3) time sequence; (b4) autocorrelation curve
    Working principle of chaotic BOCDA. (a) Schematic illustration of principle; (b) simulation of time-space distribution of chaotic SBS acoustic field in 100 m-long fiber; (c) simulation of chaotic Brillouin gain spectrum
    Fig. 2. Working principle of chaotic BOCDA. (a) Schematic illustration of principle; (b) simulation of time-space distribution of chaotic SBS acoustic field in 100 m-long fiber; (c) simulation of chaotic Brillouin gain spectrum
    Experimental setup diagram of chaotic Brillouin optical correlation-domain analysis technology
    Fig. 3. Experimental setup diagram of chaotic Brillouin optical correlation-domain analysis technology
    Temperature demodulation by chaotic BGS. (a) Measured BGSs at different positions and temperatures; (b) linear relationship between BFS and temperature
    Fig. 4. Temperature demodulation by chaotic BGS. (a) Measured BGSs at different positions and temperatures; (b) linear relationship between BFS and temperature
    Results of distributed temperature measurement[49]. (a) Chaotic BGS distribution along the FUT; (b) BFS distribution along the FUT
    Fig. 5. Results of distributed temperature measurement[49]. (a) Chaotic BGS distribution along the FUT; (b) BFS distribution along the FUT
    Distribution map of autocorrelation coefficient at external cavity feedback delay position under different injection currents and feedback strengths[50]
    Fig. 6. Distribution map of autocorrelation coefficient at external cavity feedback delay position under different injection currents and feedback strengths[50]
    Schematic diagram of time-gated system. (a) Technical principle; (b) experimental setup
    Fig. 7. Schematic diagram of time-gated system. (a) Technical principle; (b) experimental setup
    BGS comparisons of chaotic BOCDA systems with and without time-gated scheme at different fiber positions[51]. (a) 5.0 km; (b) 8.5 km; (c) 10.0 km; (d) SBR as a function of fiber position
    Fig. 8. BGS comparisons of chaotic BOCDA systems with and without time-gated scheme at different fiber positions[51]. (a) 5.0 km; (b) 8.5 km; (c) 10.0 km; (d) SBR as a function of fiber position
    Typical status of chaotic laser in bandwidth adjustment process[52]. (a1)‒(c1) Radio frequency spectra; (a2)‒(c2) autocorrelation traces; (a3)‒(c3) autocorrelation center peaks and their Gaussian fitting curves
    Fig. 9. Typical status of chaotic laser in bandwidth adjustment process[52]. (a1)‒(c1) Radio frequency spectra; (a2)‒(c2) autocorrelation traces; (a3)‒(c3) autocorrelation center peaks and their Gaussian fitting curves
    Comparisons of BGS under different data acquisition methods in millimeter-level-spatial-resolution chaotic BOCDA system[52]. (a) OPM-based scheme; (b) LIA-based scheme
    Fig. 10. Comparisons of BGS under different data acquisition methods in millimeter-level-spatial-resolution chaotic BOCDA system[52]. (a) OPM-based scheme; (b) LIA-based scheme
    Results of distributed strain measurement in millimeter-level-spatial-resolution chaotic BOCDA system[52]. (a) BGS along the FUT; (b) BFS curve along the FUT
    Fig. 11. Results of distributed strain measurement in millimeter-level-spatial-resolution chaotic BOCDA system[52]. (a) BGS along the FUT; (b) BFS curve along the FUT
    Principle of single-slope-assisted technology. (a) Schematic diagram of single-slope-assisted technology; (b) conversion coefficient between Brillouin amplitude and strain value[54]
    Fig. 12. Principle of single-slope-assisted technology. (a) Schematic diagram of single-slope-assisted technology; (b) conversion coefficient between Brillouin amplitude and strain value[54]
    Time traces and sine-fitted curves under different dynamic strains[54]. (a) 0‒100 µε; (b) 0‒1000 µε; (c) 0‒1200 µε; (d) 0‒1400 µε
    Fig. 13. Time traces and sine-fitted curves under different dynamic strains[54]. (a) 0‒100 µε; (b) 0‒1000 µε; (c) 0‒1200 µε; (d) 0‒1400 µε
    Measurement results of DSA-CBOCDA system[57]. (a) Measurement accuracy of static strain; (b) static strain resolution; (c) measurement accuracy of dynamic strain; (d) dynamic strain resolution
    Fig. 14. Measurement results of DSA-CBOCDA system[57]. (a) Measurement accuracy of static strain; (b) static strain resolution; (c) measurement accuracy of dynamic strain; (d) dynamic strain resolution
    CategoryOptimal resultsMain drawback
    Spatial resolution at sensing rangeSensing range at spatial resolutionMeasurement speed
    Sine-FM BOCDA1.6 mm at 5 m3552.1 km at 7 cm45dynamic strain: 20 kHz46bandwidth predicament;higher cost and complexity
    Phase-coded BOCDA0.64 mm at 2.8 m3717.5 km at 8.3 mm42localization: 185 points /s43high-rate modulation;higher cost and complexity
    ASE-based BOCDA0.8 mm at 5 cm385 cm at 4 mm34time consuming34poor SNR and practicality;limited sensing range
    Chaotic BOCDA3.5 mm at 165 m5210.2 km at 9 cm51dynamic strain:~5 Hz54time consuming;inconvenient of positioning
    Table 1. Research progress of BOCDA
    Yahui Wang, Le Zhao, Qian Zhang, Lijun Qiao, Tao Wang, Jianzhong Zhang, Mingjiang Zhang. Progress in Chaotic Brillouin Optical Correlation-Domain Analysis[J]. Laser & Optoelectronics Progress, 2021, 58(13): 1306011
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