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研究生:顏鉑秀
研究生(外文):Yen, Po-Hsiu
論文名稱:腔內梳狀濾波高重複率鎖模摻鉺光纖雷射之研究
論文名稱(外文):Study of high repetition rate mode locked Er doped fiber lasers with intra cavity comb filtering
指導教授:賴暎杰
指導教授(外文):Lai, Yin-Chieh
口試委員:謝文峰鄒志偉項維巍
口試委員(外文):Hsieh, Wen-FengChow, Chi-WaiHsiang, Wei-Wei
口試日期:2019-06-24
學位類別:碩士
校院名稱:國立交通大學
系所名稱:光電工程研究所
學門:工程學門
學類:電資工程學類
論文種類:學術論文
論文出版年:2019
畢業學年度:107
語文別:英文
論文頁數:52
中文關鍵詞:光纖雷射高重複率鎖模腔內梳狀濾波
外文關鍵詞:high repetition rate mode lockedEr doped fiber lasersintra cavity comb filtering
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本論文中,我們成功地實現了重複率高達 100 GHz 和 250 GHz 的脈衝雷射,透過 sigma 型式的雷射腔體,使得光得以保持單一偏振態,從而得到極度穩定的 100 GHz 脈衝序列,更進一步透過簡單的 回授控制,使得長期的雷射輸出功率變動值可以降低至 0.1 % 左右。而另一個 250 GHz的鎖模雷射則使用了高功率的摻鉺光纖放大器作為泵浦 並且使用矽環形共振器 來濾波,透過外部注入一個窄頻寬的 連續式雷射,可以有效的壓制超模所造成的擾動,進而大幅的提升自相關儀所量測到的脈衝 對比度。在這兩個不同架構的雷射中都使用了好幾百公尺的高非線性光纖來提供充足的非線性效應,像是自相位調變和四波混頻等。透過光譜儀、自相關儀和射頻頻譜儀等設備的使用,我們詳細探討了這兩種雷射的重要特性。
In the thesis work two high repetition rate fiber lasers up to 100 GHz and 250 GHz are successfully demonstrated. By utilizing a sigma type laser cavity, a highly stable 100 GHz fiber laser is achieved, thanks to the polarization maintaining cavity design. Moreover, through a simple feedback control loop, the long term output power variation is lowered to the level of 0.1 %. Another 250 GHz mode-locking laser is pumped by a high power EDFA and filtered through a silicon-microring resonator in the cavity. The autocorrelation trace is significantly improved by injecting a narrow bandwidth CW laser, which is capable of suppressing the super-mode noises. Both laser schemes require a section of several hundred meters of high nonlinearity fiber to provide the sufficient nonlinear effects of self-phase modulation and four-wave mixing. The characteristics of both laser are investigated in details by the measurement of optical spectrum, autocorrelation trace and RF spectrum.
Acknowledgment..………………………………..………….…………………………………….……….I
摘要
…………………………………………………..………………………………………………….………II
Abstract…………………………………………………..……………………………………………………III
Contents…………………………………………………..………………………………………….…………IV
Chapter 1 Introduction
1.1 Overview…………………………………………………………………………………………..…1
1.2 Motivation………………………………………………………….………………………………..3
1.3 Organization of the thesis…….………………………………………………….…………..4
Chapter2 Theories
2.1 Comb filters………………………………………………….....…………………………………5
2.1.1 Fabry Perot etalon………………………………………….…………………………6
2.1.2 Silicon micro ring resonator…………………………………………………….7
2.2 Mode matching and super mode noises………………………………………………..9
2.3 Self heterodyne measurement……………………………………….………………….11
2.4 Nonlinear effect……………………………………………………………………………….13
2.4.1 Self phase modulation…………………………………….………………………13
2.4.2 Four wave mixing………………………………………………………………….15
V
Chapter 3 Experimental setup and results
3.1 100 GHz mode--locked PM sigma type fiber laser…………………………..17
3.1.1 Laser configuration………………………………..…………………………….…18
3.1.2 Results of the hybrid cavity……………………………………….………20
3.1.3 Results of the passive cavity…………………..…………………….……23
3.2 Silicon micro--ring high power EDFA cavity..…………………………………32
3.2.1 Laser configuration………………………………..…………………………….…33
3.2.2 Micro--ring measurement………………………………………………….………34
3.2.3 Experimental result……………………………………..…………………….……37
Chapter 4 Conclusion and the future work
4.1 Conclusion……………………………………………………….………………………………..45
4.2 Future work………………………………………………………….....………………………..46
References………………………………………………………….………………………………………….48
[1] R.J. Mears, L. Reekie, I.M. Jauncey, and D.N. Payne, “Low noise erbium doped fibre amplifier operating at 1.54μm,” Electron. Lett. 23, 1026 1028 (1987).
[2] G. Sobon, J. Sotor, and K. M. Abramski, “All polarization maintaining femtosecond Er doped fiber laser mode locked by graphene saturable absorber,” Laser Phys. Lett. 9, 581 (2012).
[3] A. Martinez, Z. Sun, “Nanotube and graphene saturable absorbers for fibre lasers,” Nat. Photon 7, 842 845 (2013).
[4] Q. Bao, H. Zhang, Y. Wang, Z. Ni, Y. Yan, Z. X. Shen, K. P. Loh and D. Y. Tang, “Atomic‐Layer Graphene as a Saturable Absorber for Ultrafast Pulsed Lasers,” Adv. Functional Mater. 19, 3077 3083 (2009).
[5] K. Kieu and F. W. Wise, “All fiber normal dispersion femtosecond laser,” Opt. Express 16, 11453 (2008).
[6] S.Y. Set, H. Yaguchi, Y. Tanaka and M. Jablonski, “Laser mode locking using a saturable absorber incorporating carbon nanotubes,” J. Lightwave Technol. 22, 51 56 (2004).
[7] S. Yamashita, Y. Inoue, S. Maruyama, Y. Murakami, H. Yaguchi, M. Jablonski, and S. Y. Set “Saturable absorbers incorporating carbon nanotubes
49
directly synthesized onto substrates and fibers and their application to mode--locked fiber lasers,” Opt. Lett. 29, 1581--1583 (2004).
[8] M. E. Fermann, F. Haberl, M. Hofer, and H. Hochreiter, “Nonlinear amplifying loop mirror,” Opt. Lett. 15, 752 (1990).
[9] I. N. Duling, “All--fiber ring soliton laser mode locked with a nonlinear mirror,” Opt. Lett. 16, 539--541 (1991).
[10] C. Hou--Ren., L. Kuei--Huei, T. Chih--Ya, W. Hsiao--Hua, W. Chih--Hsuan, C. Chieh--Han, C. Yu--Chieh, L. Gong--Ru, and H. Wen--Feng, “12 GHz passive harmonic mode--locking in a 1.06 μm semiconductor optical amplifier--based fiber laser with figure--eight cavity configuration,” Opt. Lett.38, 845--847 (2013).
[11] F. Amrani, A. Haboucha, M. Salhi, H. Leblond, A. Komarov, Ph. Grelu, and F. Sanchez, “Passively mode--locked erbium--doped double--clad fiber laser operating at the 322nd harmonic,” Opt. Lett. 34, 2120 (2009).
[12] V.J. Matsas, T.P. Newson, D.J. Richardson and D.N. Payne, “Selfstarting passively mode--locked fibre ring soliton laser exploiting nonlinear polarisation rotation,” Electron. Lett. 28, 1391--1393 (1992).
[13] M. E. Fermann, M. Hofer, F. Haberl, A. J. Schmidt, and L. Turi, “Additive--pulse--compression mode locking of a neodymium fiber laser,” Opt. Lett. 16, 244--246 (1991).
50
[14] S. Y. Wu, W. W. Hsiang, and Y. Lai, “Synchronous--asynchronous laser mode--locking transition,” Physical review A 92, 013848 (2015).
[15] K. Bagnell, A. Klee, P. J. Delfyett, J. J. Plant, and P. W. Juodawlkis, “Demonstration of a highly stable 10 GHz optical frequency comb with low timing jitter from a SCOWA--based harmonically mode--locked nested cavity laser,” Opt. Lett. 43, 2396--2399 (2018).
[16] K. W. Holman, D. J. Jones, D. D. Hudson, and J. Ye, “Precise frequency transfer through a fiber network by use of 1.5--μm mode locked sources,” Opt. Lett. 29, 1554−1156 (2004).
[17] L. S. Ma, Z. Y. Bi, A. Bartels, L. Robertsson, M. Zucco, R. S. Windeler, G. Wilpers, C. Oates, L. Hollberg, and S. A. Diddams, “Optical frequency synthesis and comparison with uncertainty at the 10−19 level,” Science 303, 1843−1845 (2004).
[18] G. Meloni, G. Berrettini, M. Scaffardi, A. Bogoni, L. Poti, and M. Guglielmucci, “250--times repetition frequency multiplication for 2.5 THz clock signal generation,” Electron. Lett. 41, 1294––1295 (2005).
[19] T. M. Fortier, M. S. Kirchner, F. Quinlan, J. Taylor, J. C. Bergquist, T. Rosenband, N. Lemke, A. Ludlow, Y. Jiang, C. W. Oates, and S. A. Diddams, Nat. Photonics 5, 425 (2011).
51
[20] C. Wu, and N. K. Dutta, “High--repetition--rate optical pulse generation using a rational harmonic mode--locked fiber laser,” IEEE J. Quantum Electron. 36, 145––150 (2000).
[21] M. Quiroga--Teixeiro, C. Balslev Clausen, M. P. Sorensen, P. L. Christiansen, and P. A. Andrekson, “Passive mode locking by dissipative four--wave mixing,” J. Opt. Soc. Am. B 15, 1315 (1998).
[22] S. Gee, F. Quinlan, S. Ozharar and P.J. Delfyett, “Simultaneous optical comb frequency stabilization and super--mode noise suppression of harmonically mode--locked semiconductor ring laser using an intracavity etalon,” IEEE Photonics Technol. Lett. 17, 199 -- 201 (2005).
[23] A. Pasquazi, M. Peccianti, B. E. Little, S. T. Chu, D. J. Moss, and R. Morandotti, “Stable, dual mode, high repetition rate mode--locked laser based on a microring resonator,” Opt. Express 20, 27355--27363 (2012).
[24] E. Yoshida, and M. Nakazawa, “Low--threshold 115--GHz continuous--wave modulational--instability erbium--doped fiber laser,” Opt. Lett. 22, 1409––1411 (1997).
[25] L. G Yang, S. S. Jyu, C. W. Chow, C. H. Yeh, C. Y. Wong, H. K. Tsang, and Y. Lai, “A 110 GHz passive mode--locked fiber laser based on a nonlinear silicon--micro--ring--resonator,” Laser Phys. Lett. 11, 065101 (2014).
52
[26] J. Lhermite, D. Sabourdy, A. D. Berthelemot, V. Kermene, A. Barthelemy, and J. L. Oudar, “Tunable high--repetition--rate fiber laser for the generation of pulse trains and packets,” Opt. Lett. 32, 1734− 1736 (2007).
[27] S. M. Wang, and Y. Lai, “Generation of 100 GHz pulse train from a phase modulated hybrid mode--locked Er--fiber laser with an intra--cavity etalon,” in OptoElectronics and Communications Conference (OECC) held jointly with International Conference on Photonics in Switching (PS) (IEEE, Niigata, Japan, 2016), WA2--53.
[28] S. S. Jyu, L. G. Yang, C. Y. Wong, C. H. Yeh, C. W. Chow, H. K. Tsang, and Y. Lai, “250-GHz passive harmonic mode-locked Er-doped fiber laser by dissipative four-wave mixing with silicon-based micro-ring,” IEEE Photonics J. 5, 7 (2013).
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