簡易檢索 / 詳目顯示

研究生: 謝鎧任
論文名稱: 以方波光源注入波長增益競爭之摻鉺光纖共振腔
Dual-Wavelength Pulse Generation from Gain Competition by Injecting Square-Wave Light Signal into Erbium-Doped Fiber Cavity
指導教授: 王立康
口試委員: 呂海涵
林恭如
王立康
學位類別: 碩士
Master
系所名稱: 電機資訊學院 - 光電工程研究所
Institute of Photonics Technologies
論文出版年: 2013
畢業學年度: 101
語文別: 中文
論文頁數: 51
中文關鍵詞: 摻鉺光纖脈衝雷射幫浦增益競爭光纖光柵費比-培洛雷射二極體共振腔回饋
外文關鍵詞: FPLD, FBG
相關次數: 點閱:2下載:0
分享至:
查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報
  • 本論文將會以費比-培洛雷射二極體所構成之共振腔產生的方波光源注入增益競爭之共振腔,藉以產生兩種不同波長(1550、1555nm)的光並以交替激射形式輸出。增益競爭之共振腔部分則是在兩光纖光柵前分別放置摻鉺光纖作增益競爭,再以10/90之光耦合器之10%輸出,90%打回光纖光柵作共振,最後改變pump雷射之功率來調變輸出波長。
    雷射二極體所構成之共振腔是以函數產生器之方波電壓訊號輸入二極體驅動器,再輸入雷射二極體產生多模態的雷射,而後以摻鉺光纖放大訊號並由光纖光柵選取所需波長,並回饋注入原雷射二極體作反饋以讓系統產生共振雷射光。將此雷射二極體所構成之共振雷射光注入前面所述的增益競爭之共振腔以產生兩波長交替激射(lasing)。
    最後再討論與預期會產生類似方波之輸出訊號不一樣的地方,分別以注入光之光功率、重複率、占空因數(duty cycle)與在增益競爭之共振腔的幫浦(pump)雷射功率,這些因數會對共振腔之輸出造成什麼影響來作討論。


    第一章 序論 1 1.1研究背景 1 1.2研究動機 3 第二章 原理 4 2.1摻鉺光纖放大器之原理 4 2.2摻鉺光纖雷射(Erbium-doped fiber laser , EDFL)之原理 6 2.3費比-培洛雷射二極體之原理 7 2.4光纖布拉格光柵(Fiber Bragg grating , FBG)之原理 9 2.5 其他光學被動元件介紹 11 第三章 實驗架構與結果討論 13 3.1 增益競爭之共振腔的結構與注入CW雷射 13 3.2 脈衝雷射之製作 24 3.3以脈衝雷射注入增益競爭之共振腔 30 第四章 結論與未來展望 45 參考文獻 46

    [1] Hyo Sang Kim, Seok Hyun Yun, Hyang Kyun Kim, Namkyoo Park, and Byoung Yoon Kim, “Actively gain-flattened erbium-doped fiber amplifier over 35 nm by using all-fiber acoustooptic tunable filters,” IEEE Photonics Technology Letters,Vol. 10, No. 6, pp. 790-792, 1998.
    [2] Naveen Kumar, M. R. Shenoy, and B. P. Pal, “A standard fiber-based loop mirror as a gain-flattening filter for erbium-doped fiber amplifiers,” IEEE Photonics Technology Letters,Vol. 17, No. 10, pp. 2056-2058, 2005.
    [3] Ryun Kyung Kim, Suho Chu, and Young-Geun Han, “Stable and widely tunable single-longitudinal-mode dual-wavelength erbium-doped fiber laserfor optical beat frequency generation,” IEEE Photonics Technology Letters,Vol.24,No.6, pp. 521-523, 2012.
    [4] Yu Yao, Xiangfei Chen, Yitang Dai, and Shizhong Xie,, “Dual-wavelength erbium-doped fiber laser with a simple linear cavity and its application in microwave generation,” IEEE Photonics Technology Letters,Vol. 18, No. 1, pp. 187-189, 2006.
    [5] L. Talaverano, S. Abad, S. Jarabo, and M. López-Amo, “Multiwavelength fiber laser sources with Bragg-grating sensor multiplexing capability,” Journal of Lightwave Technology,Vol. 19, No. 4, pp. 553-558, 2001.
    [6] Xiaoying He, Xia Fang, Changrui Liao, D. N. Wang,, “A tunable and switchable single-longitudinal-mode dual-wavelength fiber laser with a simple linear cavity,” Optics Express,Vol. 17, Iss. 24, p. 21773–21781, 2009.
    [7] Shilong Pan,Xiaofan Zhao, and Caiyun Lou, “Switchable single-longitudinal-mode dualwavelength erbium-doped fiber ring laser incorporating a semiconductor optical amplifier,” Optics Letters,Vol. 33, No. 8, pp. 764-766, 2008.
    [8] N. Park, J. W. Dawson, K. J. Vahala, and C. Miller, “All-fiber,low-threshold, widely tunable single-frequency, erbium-doped fibe rring laser with a tandem fiber Fabry-Perot filter,” Appl. Phys. Lett., Vol. 57,No. 19, pp. 2369-2371, 1991.
    [9] Xia Fang and D. N. Wang, “Wavelength-tunable optical short pulses with high sidemode suppression ratio generated by use of bi-EDFA,” J. Opt. Soc. Am. B,Vol. 25, No. 11, pp. 1926-1930, 2008.
    [10] J.W. Chen , D.N. Wang, “Wavelength tunable optical short pulse generation by self-seeding of a gain-switched Fabry–Perot laser diode with extended wavelength-tuning range,” Optics Communications, pp. 345-350, 2003.
    [11] Sun Hyok Chang, In Kag Hwang, Byoung Yoon Kim, and Hee Gap Park, “Widely tunable single-frequency Er-doped fiber laser with long linear cavity,” IEEE Photonics Technology Letters,Vol. 13, No. 4, pp. 287-289, 2001.
    [12] T.C. Teyo, V. Sinivasagam, M.K. Abdullah, H. Ahmad, “An injection-locked erbium-doped fibre ring laser,” Optics & Laser Technology, pp. 493-496, 1999.
    [13] P. D. Dragic, “Analytical model for injection-seeded erbium-doped fiber ring lasers,” IEEE Photonics Technology Letters,Vol. 17, No. 8, pp. 1629-1631, 2005.
    [14] Qinghe Mao and John W. Y. Lit, “Switchable multiwavelength erbium-doped fiber laser with cascaded fiber grating cavities,” IEEE Photonics Technology Letters,Vol. 14, No. 5, pp. 612-614, 2002.
    [15] Jeng-Bin Tang, Kai-Jein Hsieh, and Likarn Wang, “Wavelength switching of erbium-doped fiber laser by optical injection into overlapped laser cavities,” Jpn. J. Appl. Phys.,Vol.51, pp. 102701-1-102701-5 , 2012.
    [16] Bo-Hun Choi, Hyo-Hoon Park, Moojung Chu, and Seung Kwan Kim, “High-gain coefficient long-wavelength-band erbium-doped fiber amplifier using 1530-nm band pump,” IEEE Photonics Technology Letters,Vol. 13, No. 2, pp. 109-111, 2001.
    [17] Bo Dong, Jianzhong Hao, Junhao Hu, and Chin-Yi Liaw, “Wide pulse-repetition-rate range tunable nanotube Q-switched low threshold erbium-doped fiber laser,” IEEE Photonics Technology Letters,Vol. 22, No. 24, pp. 1853-1855, 2010.
    [18] M. Delgado-Pinar, D. Zalvidea, A. Diez, P. Perez-Millan, and M. Andres, “Q-switching of an all-fiber laser by acousto-optic modulation of a fiber Bragg grating,” Optics Express,Vol. 14, Issue 3, pp. 1106-1112, 2006.
    [19] Luis Escalante-Zarate, Yuri O. Barmenkov, José L. Cruz, and Miguel V. Andrés, “Q-switch modulator as a pulse shaper in Q-switched fiber lasers,” Journal of Lightwave Technology,Vol. 24, No. 4, pp. 312-314, 2012.
    [20] Yutaka Fukuchi and Joji Maeda, “Stable and wavelength-tunable high-speed short pulse generation from a rational harmonic mode-locked short-cavity fiber laser using a bismuth-based erbium-doped fiber and a bismuth-based nonlinear fiber,” OSA / CLEO/QELS, pp. 1-2, 2010.
    [21] Lawrence R. Chen,Alan L. K. Cheng,Chester Shu,Serge Doucet and Sophie LaRochelle, “Mode-locked, multi-wavelength Erbium-doped fiber laser with 25 Ghz spacing,” Lasers and Electro-Optic/CLEO, pp. 1-2, 2007.
    [22] Peng-Chun Peng, Wei-Ren Peng, Jia-He Lin, Wen-Piao Lin, and Sien Chi, “Generation of wavelength-tunable optical pulses using EDFA as external-injection light source and amplifier for Fabry-Pérot laser diode,” IEEE Photonics Technology Letters,Vol. 16, No. 11, pp. 2553-2555, 2004.
    [23] F. Hirabayashi, K. Igawa, Y. Tsuda and A. Otani, “Short optical pulse generator with function of fast wavelength sweeping,” OSA/OFC, 2006.
    [24] Wei Li ,Yong-wei Li ,Xing-de Han,guo-qing Yu, “The study of enhancing temperature sensitivity for FBG temperature sensor,” Proceedings of the Eighth International Conference on Machine Learning and Cybernetics, pp. 2746-2749, 2009.
    [25] Ginu Rajan, Dean Callaghan, Yuliya Semenova, Mark McGrath, Eugene Coyle, and Gerald Farrell, “A Fiber Bragg Grating-Based All-Fiber Sensing System for Telerobotic Cutting Applications,” IEEE Sensors Journal,Vol. 10, No. 12, pp. 1913-1919, December 2010.
    [26] Chih-Wei Lai, Yu-Lung Lo, Jiahn-Piring Yur, and Chin-Ho Chuang, “Application of fiber Bragg grating level sensor and Fabry-Pérot pressure sensor to simultaneous measurement of liquid level and specific gravity,” IEEE Sensors Journal,Vol. 12, No. 4, pp. 827-831, 2012.
    [27] Piotr Myslinski, Member, IEEE, Dung Nguyen and Jacek Chrostowski, “Effects of concentration on the performance of erbium-doped fiber amplifiers,” Journal of Lightwave Technology,Vol. 15, No. 1, pp. 112-119, 1997.
    [28] S. V. Chernikov and J. R. Taylor, “Coupled-cavity erbium fiber lasers incorporating,” Optics Letters,Vol. 18, No. 23, pp. 2023-2025, 1993.

    無法下載圖示 全文公開日期 本全文未授權公開 (校內網路)
    全文公開日期 本全文未授權公開 (校外網路)

    QR CODE