Study on the Characters of Phase-Shifted Fiber Bragg Grating in Asymmetric Perturbation and Its Application in Fiber Laser Acoustic Sensor

Yanjie ZHAO; Jiasheng NI; Faxiang ZHANG; Zhiqiang SONG; Luyan LI; Ting CHEN; Shuang LI

doi:10.1007/s13320-018-0510-0

[1] L. N. Ma, Y. M. Hu, H. Luo, and Z. L. Hu, “DFB fiber laser hydrophone with flat frequency response and enhanced acoustic pressure sensitivity,” IEEE Photonics Technology Letters, 2009, 21(17): 1280-1282.

[2] C. K. Kirkendall and A. Dandridge, “Overview of high performance fiber-optic sensing,” Journal of Physics D Applied Physics, 2004, 37(18): 197-216.

[3] S. Foster, G. Cranch, J. Harrison, A. Tikhomirov, and G. Miller, “Distributed feedback fiber laser strain sensor technology,” Journal of Lightwave Technology, 2017, 35(16): 3514-3530.

[4] W. Liu, L. N. Ma, Z. L. HU, Y. Feng, and H. Y. Yang, “Study of Rayleigh-backscattering induced coherence collapse in an asymmetric DFB FL sensor,” Photonic Sensors, 2016, 6(3): 209-213.

[5] Y. J. Zhao, Q. P. Wang, J. Chang, J. S. Ni, C. Wang, Z. H. Sun, et al., “Suppression of the intensity noise in DFB fiber lasers by self-injection locking,” Laser Physics Letters, 2012, 9(10): 739-743.

[6] F. F. Hou and M. Yang, “A novel dual-wavelength DFB fiber laser,” Optik, 2013, 124(18): 3674-3677.

[7] S. Loranger, A. Tehranchi, H. Winful, and R. Kashyap, “Realization and optimization of phase-shifted distributed feedback fiber Bragg grating Raman lasers,” Optica, 2018, 5(3): 295-302.

[8] J. S. Ni, Y. J. Zhao, C. Wang, G. D. Peng, T. Y. Liu, J. Chang, et al., “Research on linewidth characteristics and broadening mechanism of distributed feedback fiber laser,” Acta Physica Sinica, 2012, 61(8): 084205-1-084205-6.

[9] Y. J. Zhao, Q. P. Wang, J. Chang, J. S. Ni, C. Wang, P. P. Wang, et al., “Linewidth narrowing and polarization control of erbium-doped fiber laser by self-injection locking,” Laser Physics, 2011, 21(12): 2108-2111.

[10] J. A. Bucaro and H. D. Dardy, “Fiber optic hydrophone,” The Journal of the Acoustical Society of America, 1997, 62(5): 1302-1304.

[11] D. J. Hill and G. A. Cranch, “Gain in hydrostatic pressure sensitivity of coated fiber Bragg grating,” Electronics Letters, 1999, 35(15): 1268-1269.

[12] W. T. Zhang, Y. L. Liu, F. Li, and H. Xao, “Fiber laser hydrophone based on double diaphragms: theory and experiment,” Journal of Lightwave Technology, 2008, 26(10): 1349-1352.

[13] J. Z. Zhang, X. L. Li, Q. Chai, Q. Q. Hao, Q. Li, W. M. Sun, et al., “Hydrophone based on intensity modulated DFB fiber laser,” in Proceeding of IEEE Sensors, Kona, HI, USA, 2010, pp. 315-317.

[14] A. I. Azmi, I. Leung, X. B. Chen, S. L. Zhou, Q. Zhu, K. Gao, et al., “Fiber laser based hydrophone system,” Photonic Sensors, 2011, 1(3): 210-221.

[15] A. D. Kersey, K. P. Koo, and M. A. Davis, “Fiber optic Bragg grating laser sensors,” SPIE, 1994, 2292: 102-112.

[16] K. P. Koo and A. D. Kersey, “Bragg grating based laser sensors systems with interferometric interrogation and wavelength division multiplexing,” Journal of Lightwave Technology, 1995, 13(7): 1243-1249.

[17] S. Foster, A. Tikhomirov, M. Milnes, J. V. Velzen, and G. Hardy, “A fiber laser hydrophone,” SPIE, 2005, 5855: 627-630.

[18] S. Foster, A. Tikhomirov, and J. V. Velzen, “Towards a high performance fiber laser hydrophone,” Journal of Lightwave Technology, 2011, 29(9): 1335-1342.

[19] K. C. Unnikrishnan and P. Venugopalan, “Pressure compensated fiber laser hydrophone: modeling and experimentation,” Journal of the Acoustical Society of America, 2013, 134(4): 2710-2718.

[20] F. X. Launay, R. Lardat, R. Bouffaron, G. Roux, and M. Doisy, “Static pressure and temperature compensated wideband fiber laser hydrophone,” SPIE, 2013, 8794: 87940k-1-87940k-5.

[21] K. Vivek, R. Rajesh, C. V. Sreehari, S. Shamkumar, K. Shajahan, T. V. Praveen, et al., “A new approach of large diameter polymer-coated fiber laser hydrophone,” Journal of Lightwave Technology, 2017, 35(19): 4097-4104.

[22] P. G. Agrawal and S. Radic, “Phase-shifted fiber Bragg gratings and their application for wavelength demultiplexing,” Photonics Technology Letters IEEE, 1994, 6(8): 995-997.

[23] A. Tehranchi, S. Loranger, and R. Kashyap, “Engineered pi-phase-shifted fiber Bragg gratings for efficient distributed feedback Raman fiber lasers,” IEEE Journal of Quantum Electronics, 2018, 54(3): 1-7.

[24] T. Makino and J. Glinski, “Transfer matrix analysis of the amplified spontaneous emission of DFB semiconductor laser amplifiers,” IEEE Journal of Quantum Electronics, 1988, 24(8): 1507-1518.

[25] S. W. Lovseth and K. Blotekjar, “Contributions to wavelength shifts of DFB fiber lasers used as acoustic sensors in air,” SPIE, 1998, 3483: 69-73.

[26] M. Ibsen, E. Ronnekleiv, G. J. Cowle, M. O. Berendt, O. Hadeler, M. N. Zervas, et al., “Robust high power (>20 mW) all-fibre DFB lasers with unidirectional and truly single polarisation outputs,” in Proceeding of Conference of Lasers and Electro-Optics, Baltimore, MD, USA, 1999, pp. 245-246.

[27] L. Poladian, B. Ashton, W. E. Padden, A. Michie, and C. Marra, “Characterisation of phase-shifts in gratings fabricated by over-dithering and simple displacement,” Optical Fiber Technology, 2003, 9(4): 173-188.

[28] G. A. Cranch, G. M. H. Flockhart, and C. K. Kirkendall, “Distributed feedback fiber laser strain sensors,” IEEE Sensors Journal, 2008, 8(7): 1161-1172.