Author Affiliations
1National Key Laboratory of Science and Technology on Tunable Laser, Harbin Institute of Technology, Harbin, Heilongjiang 150001, China2Postdoctoral Research Station for Optical Engineering & Research Center for Space Optical Engineering, Harbin Institute of Technology, Harbin, Heilongjiang 150001, China3Heilongjiang Provincial Key Laboratory of Quantum Control, School of Measurement and Communication Engineering, Harbin University of Science and Technology, Harbin, Heilongjiang 150080, Chinashow less
Fig. 1. Phase matching. (a) Backward stimulated Brillouin scattering; (b) Forward stimulated Brillouin scattering
Fig. 2. Dispersion relation of R0,m-induced F-SBS. The bule solid lines represented the dispersion curve of acoustic waves, and the red one represented which of light wave. The shade of blue lines means the intensity of F-SBS.
Fig. 3. Transverse displacement profiles. (a) Radial mode R0,5; (b) Torsional-radial mode TR2,5
Fig. 4. Spectrum of R0,m modes induced F-SBS
Fig. 5. The schematic diagram of acoustic impedance sensing
Fig. 6. SI used to measure F-SBS
Fig. 7. The experimental set-up of F-SBS measurement based on SI. The excitation and probe light are separated by their different wavelengths
[39] Fig. 8. F-SBS in multi-core fiber. (a), (b) Transverse displacement profiles of modes R
0,7 and R
0,8; (c), (d) F-SBS spectrums measured in the inner core and outer core. The excitation light propagates in the inner core
[43] Fig. 9. F-SBS in polarization maintaining fiber. (a) Experimental set-up; (b) Measured F-SBS spectrums. The red trace is measured when the excitation light propagating in the fast axis, and probe in the slow axis; The black trace is measured in the opposite situation
[41] Fig. 10. F-SBS demodulation by LPG. (a) Schematic diagram; (b) Experimental set-up
[45] Fig. 11. Distributed F-SBS sensor based on local light phase recovery. The excitation and probe pulses are not only separated by wavelength, but also by time
[36] Fig. 12. Distributed F-SBS sensor based on local light phase recovery. (a) Distributed light intensity of 0, +1 and +2-order sidebands; (b) Phase accumulation along the fiber; (c) Distributed phase shift demodulated by differentiation; (d)~(f) Distributed F-SBS spectrums measured when the fiber under test placed in air, ethanol, and water
[36] Fig. 13. Principle of OMTDR. The energy transferred between the dual-frequency components of the pulses, and their Rayleigh scattering lights are used to demodulation
[47] Fig. 14. Distributed sensing results of OMTDR. (a)~(c) are the distributed F-SBS spectrums measured when the fiber under test placed in air, ethanol, and water
[47] Fig. 15. Schematic diagram of OMTDA
[35] Fig. 16. Schematic diagram of the fiber under test
[48] Fig. 17. Distributed results of OMTDA. (a) The energy transfer process along the fiber; (b) Distributed F-SBS gain spectrum
[48] Fig. 18. Results of acoustic impedance sensing. (a) The linewidth of spectrums along the fiber; (b) F-SBS spectrums measured in air and ethanol
[48] Fig. 19. Results of distributed diameter measurements
[12]. (a) Diameter distribution before and after etching and its comparison with the SEM results (A-F); (b) Diameter variations along the FUT; (c) Representative images of the fiber cross section at A, B, C and E captured by SEM
Fig. 20. (a) Experimental setup for polarization separation assisted OMTDA; (b) Temporal trace and frequency components of activation and probing pulses
[49] 物质名称 | 声阻抗/(kg·m−2·s−1) | F-SBS谱宽/MHz | 数据来源 | 空气 | 439.6 | 0.45 | [35]
| 酒精 | 0.93×106 | 2.21 | [35]
| 水 | 1.483×106 | 3.57 | [36]
| NaCl溶液(4%) | 1.571×106 | 3.78 | [11]
| NaCl溶液(8%) | 1.664×106 | 4.00 | [11]
| NaCl溶液(12%) | 1.763×106 | 4.24 | [11]
| 聚酰亚胺(用作涂覆层) | 3.60×106 | 8.7(2.83) | [32]
| 丙烯酸酯(用作涂覆层) | 3.39×106 | 8.16(~8) | [37]
| 二氧化硅 | 13.19×106 | \ | [32]
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Table 1. Acoustic impedance and F-SBS spectrum width of common substances