• Advanced Photonics Nexus
  • Vol. 2, Issue 3, 036011 (2023)
Yahui Wang1、2、†, Xinxin Hu1, Lintao Niu1, Hui Liu1, Jianzhong Zhang1, and Mingjiang Zhang1、2、3、*
Author Affiliations
  • 1Taiyuan University of Technology, Ministry of Education, Key Laboratory of Advanced Transducers and Intelligent Control System, Taiyuan, China
  • 2Taiyuan University of Technology, College of Physics, Taiyuan, China
  • 3Shanxi-Zheda Institute of Advanced Materials and Chemical Engineering, Taiyuan, China
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    DOI: 10.1117/1.APN.2.3.036011 Cite this Article Set citation alerts
    Yahui Wang, Xinxin Hu, Lintao Niu, Hui Liu, Jianzhong Zhang, Mingjiang Zhang. Long-range chaotic Brillouin optical correlation domain analysis with more than one million resolving points[J]. Advanced Photonics Nexus, 2023, 2(3): 036011 Copy Citation Text show less
    Schematic illustration of the chaotic BGS construction. (a) Conventional chaotic BOCDA; (b) definition of pulse ER in chaos-based scheme; (c) time-gated chaotic BOCDA system; (d) definition of the chaos PBR; (e) measurement of the noise floor along the FUT; (f) pure chaotic BGS after differential denoising.
    Fig. 1. Schematic illustration of the chaotic BGS construction. (a) Conventional chaotic BOCDA; (b) definition of pulse ER in chaos-based scheme; (c) time-gated chaotic BOCDA system; (d) definition of the chaos PBR; (e) measurement of the noise floor along the FUT; (f) pure chaotic BGS after differential denoising.
    Optimization of the chaotic BGS in simulation. (a) Time series under different pulse modulation methods; (b) measured BGSs with or without time gating; (c) BGSs at different positions in long-range system; (d) schematic of differential denoising method.
    Fig. 2. Optimization of the chaotic BGS in simulation. (a) Time series under different pulse modulation methods; (b) measured BGSs with or without time gating; (c) BGSs at different positions in long-range system; (d) schematic of differential denoising method.
    Experimental setup of the proposed long-range chaotic BOCDA.
    Fig. 3. Experimental setup of the proposed long-range chaotic BOCDA.
    The BGSs under different schemes at two positions along the FUT. (a) 13.80 km and (b) 27.53 km. (c) The SBR as a function of the fiber position.
    Fig. 4. The BGSs under different schemes at two positions along the FUT. (a) 13.80 km and (b) 27.53 km. (c) The SBR as a function of the fiber position.
    The BGS map along (a) the second half of the FUT or (b) the SMF2 without Lorentz fit. The BGS map along (c) the second half of the FUT or (d) the SMF2 with Lorentz fit.
    Fig. 5. The BGS map along (a) the second half of the FUT or (b) the SMF2 without Lorentz fit. The BGS map along (c) the second half of the FUT or (d) the SMF2 with Lorentz fit.
    The BFS accuracy at the SMF2 with different data processing methods. Standard deviation (a1) of single measurement or (a2) of the 30 independent repeated measurements before Lorentz fit; standard deviation (b1) of single measurement or (b2) of the 30 independent repeated measurements after Lorentz fit.
    Fig. 6. The BFS accuracy at the SMF2 with different data processing methods. Standard deviation (a1) of single measurement or (a2) of the 30 independent repeated measurements before Lorentz fit; standard deviation (b1) of single measurement or (b2) of the 30 independent repeated measurements after Lorentz fit.
    (a) The BFS distribution near 10 cm strain section under different strains applied; (b) the BFS as a function of the applied strain.
    Fig. 7. (a) The BFS distribution near 10 cm strain section under different strains applied; (b) the BFS as a function of the applied strain.
    The BFS distribution at the SMF2 and the zoomed view near the strain section.
    Fig. 8. The BFS distribution at the SMF2 and the zoomed view near the strain section.
    Yahui Wang, Xinxin Hu, Lintao Niu, Hui Liu, Jianzhong Zhang, Mingjiang Zhang. Long-range chaotic Brillouin optical correlation domain analysis with more than one million resolving points[J]. Advanced Photonics Nexus, 2023, 2(3): 036011
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