光纖雷射的製作大致分為兩種，線性迴路共振腔(Linear Cavity)與環形迴路共振腔(ring cavity)，而我們是利用光環流器(Circulator)和可注入式Fabry-Perot Laser Diode來達成共振腔體，利用了Bending Fiber的理論和Fabry-Perot Laser Diode的操作電壓來控制雷射的波長輸出。
ㄧ開始我們先利用摻鉺光纖放大器來產生ASE(Amplified spontaneous emission)，由於ASE是寬頻光源(Broadband light source)，將此光源做Bending，不同波長下光纖損耗分佈不同，ASE分佈被改變，將此摻鉺光纖放大器做環形迴路共振腔，形成雷射輸出的波長將落在大訊號下摻鉺光纖放大器增益最大的波段，此方法除了降低各光調變元件的成本，例如FBG(Fiber Bragg Grating)等等，現在我們想要產生多波長雷射，運用均勻介質(Homogeneous Broadening Medium)的摻鉺光纖是不行的，所以我們在共振迴路中加上Fabry-Perot Laser Diode，使得共振腔內有兩種增益介質，並利用Fabry-Perot Laser Diode的非均勻介質來產生多波長雷射，結合Bending與Fabry-Perot Laser Diode就能產生可調式單、多波長光纖雷射。

1. Likourezos, G.,” Jan. 28, 1958: A laser is born,” IEEE Spectrum , vol. 29, no. 5 , 1992 , p.43
2. 張安華, “光纖通訊與實習,”新文京開發, 民國94年
3. Pezeshki, B. Vail, E. Kubicky, J. Yoffe, G. Zou, S. Heanue, J. Epp, P. Rishton, S. Ton, D. Faraji, B. Emanuel, M. Hong, X. Sherback, M. Agrawal, V. Chipman, C. Razazan, T.,” 20-mW widely tunable laser module using DFB array and MEMS selection,” Photonics Technology Letters, vol. 14, no. 10, 2002, pp. 1457-1459
4. A. D. Kersey, T. A. Berkoff, and W. W. Morey ,”Multiplexed fiber Bragg grating strain-sensor system with a fiber Fabry - Perot wavelength filter,” Optics Letters, vol. 18, no. 16, p. 1370
5. Schell, M.; Huhse, D.; Utz, W.; Kaessner, J.; Bimberg, D.; Tarasov, I.S.,” Jitter and dynamics of self-seeded Fabry-Perot laser diodes,” IEEE Journal of Selected Topics in Quantum, vol. 1, no. 2, 1995, pp.528-534
6. PC Peng, HY Tseng, S Chi,” A tunable dual-wavelength erbium-doped fiber ring laser using a self-seeded Fabry-Perot laser diode,” vol. 15, no. 5, pp. 661-663
7. Chow, K.K.; Shu, C. ,” Spectrally resolved analysis of fast tuning in single-mode pulses generated from mutually injection-seeded Fabry-Perot laser diodes,” IEEE Photonics Technology Letters , vol. 12, no. 11, 2000 , pp. 1444-1446
8. Dodds, D.E. Sieben, M.J.,” Fabry-Perot laser diode modeling,” IEEE Photonics Technology Letters, vol. 7, no. 3, 1995, pp. 254-256
9. 林螢光, “光電子學 : 原理.元件與應用,”全華, 1999
10. Desurvire, Emmanuel; Zervas, Michael N.,” Erbium-Doped Fiber Amplifiers: Principles and Applications,” Physics Today, vol. 48, no. 2, 1995 p. 56
11. Giles, C.R. Desurvire, E.,” Modeling erbium-doped fiber amplifiers,” Lightwave Technology, vol. 9, no. 2, 1991, pp.271-283
12. Sun, Y. Zyskind, J.L. Srivastava, A.K.,” Average inversion level, modeling, and physics of erbium-dopedfiber amplifiers,” IEEE Journal of selected topics in quantum electronics, vol. 3, no. 4, 1997, pp. 991-1007
13. PC Becker, NA Olsson, JR Simpson,” Erbium-doped fiber amplifiers: fundamentals and technology,” ACADEMIC, 1999
14. Ono, H. Yamada, M. Kanamori, T. Sudo, S. Ohishi, Y.,” 1.58-μm band gain-flattened erbium-doped fiber amplifiers forWDM transmission systems,” Lightwave Technology, vol. 17, no. 3, 1999, pp. 490-496
15. Faustini, L. Martini, G. ,” Bend loss in single-mode fibers,” Lightwave Technology, vol. 15, no. 4, 1997, pp. 671-679
16. Kevin Cyrus Robinson, Zionsville, Pa ,Patent Number 6137941
17. Yamashita, S. ,” Widely tunable erbium-doped fiber ring laser covering both C-bandand L-band,” IEEE Journal of selected topics in quantum electronics, vol. 7, no. 1, 2001, pp. 41-43
18. Xinyong Dong, Hwa-Yaw Tam, Bai-Ou Guan, Chunliu Zhao, and Xiaoyi Dong,” High power erbium-doped fiber ring laser with widely tunable range over 100 nm ,” Optics Communications, vol. 224, no. 4, 2003, pp. 295-299