1) stimulated raman scattering
受激拉曼散射效应
1.
Study of Stimulated Raman Scattering in Optical Fiber Gratings;
光纤光栅受激拉曼散射效应的研究
2) SRS between channels
信道间受激拉曼散射效应
3) SRS
受激拉曼散射
1.
Analysis of SRS induced crosstalk in SM fiber WDM transmission;
单模光纤WDM传输中受激拉曼散射引起的串扰分析
2.
Investigating of SRS and luminescence of ZnWO_4 crystals;
钨酸锌晶体的受激拉曼散射和光致发光研究
3.
The Stokes spectrum in the Stimulated Raman Scattering(SRS) is very complicate.
受激拉曼散射 (SRS)的Stokes波谱线型比较复杂 ,本文采用Gauss线型近似 ,研究了多波长泵浦宽带Raman放大器的增益特性 ,并提出了宽带增益平坦的多波长泵浦方案 ,研究结果表明增益平坦程度与泵浦波的频率间隔密切相关。
4) stimulated Raman scattering
受激拉曼散射
1.
Stimulated Raman scattering and thermal stress in double clad fiber laser;
双包层光纤激光器的受激拉曼散射与热应力
2.
Stimulated Raman scattering and thermal effect in high power double clad fiber laser;
高功率双包层光纤激光器受激拉曼散射和热效应的理论研究
3.
Experimental investigations of stimulated Raman scattering in D_2 and D-2/He pumped by the Nd:YAG fourth harmonic laser;
Nd:YAG四倍频激光抽运D_2和D_2／He受激拉曼散射的实验研究
5) stimulated Raman scattering (SRS)
受激拉曼散射
1.
In this paper, a combinative technology of harmonic solid state laser and stimulated Raman scattering (SRS) has been investigated to obtain multi wavelength laser output with definite power.
研究了多谐波固体激光器在气体中的受激拉曼散射 ,获得了多波长激光输出。
2.
Based on the principle of Stimulated Raman Scattering (SRS) in fiber, the dissertation is focused on the study of Raman fiber amplifiers and multiwavelength Raman fiber lasers.
本论文基于光纤中受激拉曼散射现象的基本原理,围绕拉曼光纤放大器和多波长拉曼光纤激光器展开研究。
3.
Stimulated Raman scattering (SRS) is a stimulated-scattering process with some characteristics same to laser radiation, which can be used to generate new coherent radiation sources and has long been shown to be an important method to shift laser wavelength.
受激拉曼散射(SRS)作为一种受激散射过程,具有与激光辐射完全相同的特性,可以用于产生新的相干辐射资源,已成为激光波长变换的一种重要方法。
6) self-stimulated Raman scattering
自受激拉曼散射
补充资料：受激喇曼散射
某物质能级1与能级2之间的能量差为h墹v（见图），当频率为v的单色光入射到此介质中时,如处于能级 1的介质分子吸收一个入射光子而跃迁到某个虚能级上，并从此虚能级跃迁回到能级2上,同时发射一个频率为vs＝v-墹v的散射光子,则vs线称为喇曼散射的斯托克斯线。若处于能级 2上的分子吸收一个入射光子，随后从虚能级跃迁回到能级1上,并发射一个频率为va＝v＋墹v的散射光子，则va线称为喇曼散射的反斯托克斯线。?比肷涔馇拷先跏?,散射过程基本上是自发散射,即普通的喇曼散射。当入射光是很强的激光时，受激散射成为主导的。散射光的这种变化过程有明显的阈值。入射光强超过此阈值后,散射光的强度突然增大,并有很高的方向性、单色性和相干性。这就是受激喇曼散射。受激喇曼散射可用于物质结构的研究，同时又是产生具有新波长的激光的一种方法。基于此效应而制成的喇曼移频器，已使激光输出波长扩展到远红外和真空紫外范围。利用后向喇曼散射，可以压缩激光脉冲的宽度，从而获得极高的峰值功率。(见彩图)
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条