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偏振模色散对飞秒孤子脉冲传输的影响

The Influence of Polarization Mode Dispersion to Femtosecond Optical Soliton
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摘要 以Maxwell电磁场理论为基础,在综合考虑了高阶色散、高阶非线性、自相位调制、交叉相位调制、自变陡、脉冲内喇曼散射以及偏振模色散(PMD)等因素的基础上,推导了飞秒孤子脉冲在双折射光纤中传输的耦合非线性薛定谔方程(NLSE)。利用分步傅立叶方法对该方程进行了数值计算,通过对该系统的仿真,研究分析了PMD对飞秒孤子传输的影响。结果发现当PMD参量Dp≤0.1 ps/km1/2时,输出脉冲宽度和峰值功率相对于初始脉冲几乎不变,随着Dp值的增大,脉宽增加,峰值功率降低。当Dp≥1.0 ps/km1/2时,脉冲显著展宽,孤子的两偏振分量发生严重走离。 Based on the Maxwell electromagnetic theory, nonlinear Schroedinger equation(NLSE), which described the propagation of femtosecoad soliton pulses in fiber-optic, was induced in the presence of high-step dispersion, high-step nonlinearity, self-phase modulation, cross-phase modulation, self-steep, Roman scatter in pulse and polarization mode dispersion (PMD). With split-step Fourier transform method, some useful results about the PMD influence on femtosecond solitons have been obtained. The results indicate that while the PMD is small like the Dp ≤0.1 ps/km^1/2, the transmission system can hardly be affected by PMD. But, along with the increase of Dp, performances of femtosecond soliton system degrades quickly. If Dp ≥ 1.0 ps/km^1/2, pulses are distinctly broadened and the two polarization parts are seriously departed.
出处 《光电子技术与信息》 CAS 2006年第2期40-43,共4页 Optoelectronic Technology & Information
关键词 光纤通信 飞秒孤子脉冲 偏振模色散 非线性薛定谔方程 分步傅立叶方法 optical fiber communication femtosecond soliton pulse polarization mode dispersion (PMD) nonlinear SchrSdinger equation(NLSE) split-step Fourier transform method
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