浏览全部资源
扫码关注微信
1. 内蒙古大学 物理科学与技术学院,内蒙古 呼和浩特,010021
2. 北京京东方光电科技有限公司 北京,100080
收稿日期:2010-10-13,
修回日期:2011-03-24,
网络出版日期:2011-05-22,
纸质出版日期:2011-05-22
移动端阅览
贾维国, 杨盛际, 尹健全, 王旭颖, 张俊萍, 樊国梁. 色散位移光纤中拉曼散射与参量放大增益谱[J]. 发光学报, 2011,32(5): 487-492
JIA Wei-guo, YANG Sheng-ji, YIN Jian-quan, WANG Xu-ying, ZHANG Jun-ping, FANG Guo-liang. Gain Spectra of Raman Scattering and Parametric Amplification in Birefringence Dispersion Shifted Fiber[J]. Chinese Journal of Luminescence, 2011,32(5): 487-492
贾维国, 杨盛际, 尹健全, 王旭颖, 张俊萍, 樊国梁. 色散位移光纤中拉曼散射与参量放大增益谱[J]. 发光学报, 2011,32(5): 487-492 DOI: 10.3788/fgxb20113205.0487.
JIA Wei-guo, YANG Sheng-ji, YIN Jian-quan, WANG Xu-ying, ZHANG Jun-ping, FANG Guo-liang. Gain Spectra of Raman Scattering and Parametric Amplification in Birefringence Dispersion Shifted Fiber[J]. Chinese Journal of Luminescence, 2011,32(5): 487-492 DOI: 10.3788/fgxb20113205.0487.
由斯托克斯波和反斯托克斯波所满足的耦合微分方程
考虑泵浦波是线偏振光
其偏振方向沿
x
轴
推导出了同偏振方向受激拉曼散射和参量放大同时作用下
斯托克斯波和反斯托克斯波的增益谱。引入平行拉曼散射增益系数的洛伦兹模型
研究了色散位移光纤中斯托克斯波和反斯托克斯波的增益谱随相关参数的变化关系。结果表明
斯托克斯波与反斯托克斯波的增益谱呈现出不对称
其增益谱与三色散系数
3
无关。同时讨论了反斯托克斯波与斯托克斯波|
E
ax
/
E
sx
|的比值随频移的增加而快速衰减的变化特性。
Taking account of the coupling differential equations under the effect of Stokes and anti-Stokes for the pump wave linearly polarized and aligned with the
x
-axis direction
the gain coefficient for the Stokes and anti-Stokes have been derived from simultaneously act of stimulated Raman scattering and parametric amplification in the same
x
polarization. The Lorenz model of parallel gain coefficient is introduced in this equation. The correlation between the gain spectrum and correlative parameter studied in dispersion-shifted fiber. The conclusion shows that gain spectrum is dissymmetrical with the Stokes and anti-Stokes wave and has no relation with third-order dispersion. At the same time
the ratio of Stokes and anti-Stokes |
E
ax
/
E
sx
| increases with frequency shift
then it rapidly reduced.
Schenato L, Santagiustina M, Someda C G. Fundamental and random birefringence limitations to delay in slow light fiber parametric amplification [J]. Journal of Lightwave Technology, 2008, 26 (2-24):3721-3726.[2] Trillo S, Wabnitz S. Parametric and Raman amplification in birefringent fibers [J]. J. Opt. Soc. Am. B, 1992, 9 (7):1061-1082.[3] Chee J K, Liu J M. Polarization-dependent parametric and Raman processes in a birefringent optical fiber [J]. IEEE J. Quantum Electron., 1990, 26 (3):541-542.[4] Morgan P N, Liu J M. Parametric four-photo mixing followed by stimulated Raman scattering with optical pulses in birefringent optical fibers [J]. IEEE J. Quantum Electron., 1991, 27 (4):1011-1021.[5] Agrawal G P. Nonlinear Fiber Optics:Application of Fiber Optics [M]. Jia Dongfang, et al. Transl. 3rd ed. Beijing:Publishing House of Electronics Industry, 2002:27-30,130-133,245-249 (in Chinese).[6] Hsieh A S Y, Wong G K L, Murdoch S G, et al. Combined effect of Raman and parametric gain on single-pump parametric amplifiers [J]. Optics Express, 2007, 15 (3):8104-8114 .[7] Lin Q, Agrawal G P. Raman response function for silica fibers [J]. Optics Letters, 2006, 31 (21):3086-3088.[8] Reid D T, Sibbett W, Dudley J M, et al. Commercial semiconductor devices for two photon absorption autocorrelation of ultrashort light pulses [J]. Applied Optics, 1998, 37 (34):8142-8144.[9] Zhao Yu, Zhao Deshuang, Liu Yongzhi. Analysis of fluorescens characteristic in high-energy pulsed fiber laser [J]. Chin. J. Lumin.(发光学报), 2008, 29 (5):891-896 (in Chinese).[10] Zhong Xianqiong, Xiang Anping, Luo Li, et al. Frequency chirps and spectra of chirped Gaussian optical pulses in case of negative quintic nonlinearity [J]. Chin. J. Lumin.(发光学报), 2007, 28 (1):13-17 (in Chinese).
0
浏览量
148
下载量
1
CSCD
关联资源
相关文章
相关作者
相关机构