Generation of ultra-short optical pulse trains induced by optical perturbations in optical fibers with quintic nonlinearity

被引:0
作者
Department of Optoelectronic Technology, Chengdu University of Information Technology, Chengdu 610225, China [1 ]
机构
[1] Department of Optoelectronic Technology, Chengdu University of Information Technology
来源
Zhongguo Jiguang | 2008年 / 12卷 / 1946-1950期
关键词
Nonlinear optics; Quintic nonlinearity; Sine optical perturbation; Split-step Fourier algorithm; Ultra-short optical pulse trains;
D O I
10.3788/CJL20083512.1946
中图分类号
学科分类号
摘要
Starting from the extended nonlinear Schrdinger equation in which the quintic nonlinearity effect is included, the evolution and splitting process of continuous optical wave which is amplitude perturbed by the sine optical wave into ultra-short optical pulse trains in optical fibers is numerically simulated by adopting the split-step Fourier algorithm. The effects of the quintic nonlinearity and the modulation period of the sine optical wave on the generation and evolution of ultra-short optical pulse trains and the corresponding spectra are investigated. The results show that, in comparison with the case of cubic nonlinearity only, the positive quintic nonlinearity can shorten the optimal fiber length required to form the pulse trains and make every pulse shorter in width and higher in peak power, while the negative quintic nonlinearity takes the opposite. The sine modulation period may influence the pulse repetition rate and the optimal fiber length. With the increase of the propagation distance, every single pulse may split into two and even three sub-pulses. Moreover, some small pulses with weak peak powers may appear among the main pulses. In terms of the frequency spectra, the positive (negative) quintic nonlinearity can make the number of frequency components increase (decrease) and the spectral width wide (narrow). Depending on whether the main pulses split and the small pulses exist or not, the spectra take on different shapes.
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页码:1946 / 1950
页数:4
相关论文
共 17 条
[1]  
Nonlinear Fiber Optics & Applications of Nonlinear Fiber Optics, pp. 88-93, (2002)
[2]  
Jia W., Shi P., Yang X., Et al., Modulation instability of fiber Bragg gratings with raised cosine apodization, Chinese J. Lasers, 34, 7, pp. 930-934, (2007)
[3]  
Zhong X., Xiang A., Effects of group-velocity mismatch and cubic-quintic nonlinearity on cross-phase modulation instability in optical fibers, Chin. Opt. Lett., 5, 9, pp. 534-537, (2007)
[4]  
Cai W., Wen S., Chen L., Modulation instability in fiber grating with nonlinearity management, Acta Optica Sinica, 26, 9, pp. 1387-1391, (2006)
[5]  
Tai K., Tomita A., Jewell J.L., Et al., Generation of subpicosecond solitonlike optical pulses at 0.3 THz repetition rate by induced modulation instability, Appl. Phys. Lett., 49, 5, pp. 236-238, (1986)
[6]  
Sylvestre T., Coen S., Emplit P., Et al., Self-induced modulation instability laser revisited: Normaldispersion and dark-pulse train generation, Opt. Lett., 27, 7, pp. 482-484, (2002)
[7]  
Dianov E.M., Mamyshev P.V., Prokhorov A.M., Et al., Generation of a train of fundamental solitons at a high repetition rate in optical fibers, Opt. Lett., 14, 18, pp. 1008-1010, (1989)
[8]  
Hasegawa A., Generation of a train of soliton pulses by induced modulation instability in optical fibers, Opt. Lett., 9, 7, pp. 288-290, (1984)
[9]  
Honzatko P., Peterka P., Kanka J., Modulation instability σ-resonator fiber laser, Opt. Lett., 26, 11, pp. 810-812, (2001)
[10]  
de Matos C.J.S., Chestnut D.A., Taylor J.R., Low-threshold self-induced modulational instability ring laser in highly nonlinear fiber yielding a continuous-wave 262-GHz soliton train, Opt. Lett., 27, 11, pp. 915-917, (2002)