摘要A new means of generating all-optically high-repetition-rate pulse trains is proposed and numerically demonstrated in an optical fiber. Our numerical simulations show that, due to the modulation instability effect, the initial continuous-wave with a weak optical pulse instead of conventional weak sinusoidal modulation imposed on it can gradually evolve into high-repetition-rate pulse trains. However, the generated pulse trains take on different features from the conventional case in terms of their widths, intensities, intervals, numbers, and pedestals.
Abstract:A new means of generating all-optically high-repetition-rate pulse trains is proposed and numerically demonstrated in an optical fiber. Our numerical simulations show that, due to the modulation instability effect, the initial continuous-wave with a weak optical pulse instead of conventional weak sinusoidal modulation imposed on it can gradually evolve into high-repetition-rate pulse trains. However, the generated pulse trains take on different features from the conventional case in terms of their widths, intensities, intervals, numbers, and pedestals.
(Dynamics of nonlinear optical systems; optical instabilities, optical chaos and complexity, and optical spatio-temporal dynamics)
引用本文:
ZHONG Xian-Qiong;XIANG An-Ping. Generation of High-Repetition-Rate Pulse Trains through the Continuous-Wave Perturbed by a Weak Gaussian Pulse in an Optical Fiber[J]. 中国物理快报, 2010, 27(1): 14203-014203.
ZHONG Xian-Qiong, XIANG An-Ping. Generation of High-Repetition-Rate Pulse Trains through the Continuous-Wave Perturbed by a Weak Gaussian Pulse in an Optical Fiber. Chin. Phys. Lett., 2010, 27(1): 14203-014203.
[1] Teng H, Yun C X, Zhu J F, Han H N, Zhong X, Zhang W, Hou Xand Wei Z Y 2009 Chin. Phys. Lett. 26 113201 [2] Dai Y T and Xu C 2009 Opt. Express 17 6584 [3] Li Y X, Ji Z G, Zeng Z N, Liu J S, Ge X C, Li R X and Xu ZZ 2008 Chin. Phys. Lett. 25 3272 [4] Li Y X, Zeng Z N, Ge X C, Chen X W, Li R X and Xu Z Z 2008 Chin. Phys. Lett. 25 4296 [5] Xu S X, Gao Y X, Cai H and Li J Z 2009 Chin. Phys.Lett. 26 114209 [6] Bartels A, Dekorsy T and Kurz H 1999 Opt. Lett. 24 996 [7] Jones D J, Diddams S A, Ranka J K, Stentz A J, Windeler RS, Hall J L and Cundiff S T 2000 Science 288 635 [8] Chu S W, Liu T M, Sun C K, Lin C Y and Tsai H J 2003 Opt. Express 11 933 [9] Jeon M Y, Lee H K, Ahn J T, Kim K H, Lim D S and Lee E H1998 Opt. Lett. 23 855 [10] Gupta K K, Onodera N, Abedin K S and Hyodo M 2002 IEEE Photo. Tech. Lett. 14 284 [11] Yang S Q, Zhao C L, Li Z H, Yuan S Z and Dong X Y 2002 Chin. Phys. Lett. 19 786 [12] Yandong G, Ping S and Dingyuan T 2002 Micro. Opt.Technol. Lett. 32 320 [13] Gong Y D, Shum P, Tang D Y, Lu C, Qi Z W, Lai W J, Man WS and Tam H Y 2003 Opt. Commun. 220 297 [14] Kennedy R E, Popov S V and Taylor J R 2006 Opt.Lett. 31 167 [15] Gong Y D, Shum P, Tang D Y, Lu C and Guo X 2003 Opt.Express 11 2480 [16] Honzatko P, Peterka P and Kanka J 2001 Opt. Lett. 26 810 [17] Yoshida E and Nakazawa M 1997 Opt. Lett. 221409 [18] Hong W P 2002 Opt. Commun. 213 173 [19] Agrawal G P 1992 IEEE Photo. Technol. Lett. 4562 [20] Hasegawa A 1984 Opt. Lett. 9 288