物理学报
物理學報
물이학보
2013年
4期
233-241
,共9页
柴宏宇*%贾维国%韩凤%门克内木乐%杨军%张俊萍
柴宏宇*%賈維國%韓鳳%門剋內木樂%楊軍%張俊萍
시굉우*%가유국%한봉%문극내목악%양군%장준평
不同频率区域%保偏光纤%拉曼效应%参量放大
不同頻率區域%保偏光纖%拉曼效應%參量放大
불동빈솔구역%보편광섬%랍만효응%삼량방대
different frequency propagation regimes%polarization maintaining fibers%Raman effect%parametric amplification
根据考虑拉曼效应后的双折射光纤所满足的非线性相干耦合薛定谔方程,推导出了当沿两个偏振轴入射两束不同波长的激光脉冲时所产生的增益表达式.通过与入射相同频率的光脉冲所产生增益的对比,在考虑拉曼效应的情况下,讨论了入射不同频率光脉冲对增益谱的影响.结果表明,在正常色散区和反常色散区,当输入两束激光脉冲频率不同时,增益谱较输入相同频率激光脉冲时产生了明显的变化,其外侧的斯托克斯部分和反斯托克斯部分增益峰,随着群速度失配的增加强度明显加强、偏离中心频率,可以用于提取太赫兹脉冲.当两偏振模处于不同色散区时,增益谱与不考虑拉曼效应时也存在明显的不同,增益谱的对称性遭到破坏,斯托克斯部分的增益峰强度要明显高于反斯托克斯部分.
根據攷慮拉曼效應後的雙摺射光纖所滿足的非線性相榦耦閤薛定諤方程,推導齣瞭噹沿兩箇偏振軸入射兩束不同波長的激光脈遲時所產生的增益錶達式.通過與入射相同頻率的光脈遲所產生增益的對比,在攷慮拉曼效應的情況下,討論瞭入射不同頻率光脈遲對增益譜的影響.結果錶明,在正常色散區和反常色散區,噹輸入兩束激光脈遲頻率不同時,增益譜較輸入相同頻率激光脈遲時產生瞭明顯的變化,其外側的斯託剋斯部分和反斯託剋斯部分增益峰,隨著群速度失配的增加彊度明顯加彊、偏離中心頻率,可以用于提取太赫玆脈遲.噹兩偏振模處于不同色散區時,增益譜與不攷慮拉曼效應時也存在明顯的不同,增益譜的對稱性遭到破壞,斯託剋斯部分的增益峰彊度要明顯高于反斯託剋斯部分.
근거고필랍만효응후적쌍절사광섬소만족적비선성상간우합설정악방정,추도출료당연량개편진축입사량속불동파장적격광맥충시소산생적증익표체식.통과여입사상동빈솔적광맥충소산생증익적대비,재고필랍만효응적정황하,토론료입사불동빈솔광맥충대증익보적영향.결과표명,재정상색산구화반상색산구,당수입량속격광맥충빈솔불동시,증익보교수입상동빈솔격광맥충시산생료명현적변화,기외측적사탁극사부분화반사탁극사부분증익봉,수착군속도실배적증가강도명현가강、편리중심빈솔,가이용우제취태혁자맥충.당량편진모처우불동색산구시,증익보여불고필랍만효응시야존재명현적불동,증익보적대칭성조도파배,사탁극사부분적증익봉강도요명현고우반사탁극사부분.
The expression of gain is derived from nonlinear Schr¨odinger equation with consideration of raman effect when two laser pulses with different wavelengths are emitted into birefringence fiber along two polarization axes. The gain characteristic input laser pulses of different frequencies are revealed by comparing the laser pulses of identical frequency. The result show that the gain spectra will apparently differ when input laser pulses have different frequencies in normal dispersion regime and anomalous dispersion regime. The intensities of outboard gain peak about stokes part and anti-stokes part increase and frequency deviates from central frequency as group velocity mismatch increases. Therefore, the THz pulse can be extracted. The gain spectrum will be apparently different from that with no Raman effect taken into account, when the two polarization modes, are in different dispersion regimes. The symmetry of gain spectrum will be damaged. The intensity of gain peak of stokes is apparently stronger than the peak of anti-stoke.