拉曼激光器基于受激的拉曼散射，通过它能够得到固体激光器不能直接发射的波长。它的基本组成部分有高压气体光电盒和谐振腔光学器件。如果以高功率激光器泵浦完全被动的器件就有部分激光波长转换为较长的波长。非常光波长的转换取决于发生SRS的气体。
The pumping source is a 1427.2nm Raman laser with tunable output power. The pumped fiber length is 25.2 kilometer.
泵浦源采用中心波长为1427.2nm，输出功率可调的拉曼激光器，光纤长度为25.2公里。
参考来源 - 分布式光纤拉曼放大器的模拟及优化·2,447,543篇论文数据，部分数据来源于NoteExpress
近年来，利用晶体材料的受激拉曼散射(SRS)效应建立的全固态拉曼激光器成为引人瞩目的亮点。
In recent years, much attention has been paid to the designing and operation of all-solid-state Raman lasers based on the stimulated Raman scattering (SRS) of crystals.
而光纤拉曼激光器(RFL)又作为FRA的泵浦源，它与光纤的耦合损耗小，可以实现泵浦与放大的良好兼容。
While optical fiber Raman laser (RFL) can be a good pump of FRA. The coupling coefficient between FRL and the transmission fiber is very small, so the pump and the amplifier can be compatible easily.
利用线性模型求出了级联掺磷拉曼光纤激光器各级光输出功率的显式近似解。
In this paper, the approximate explicit solution of optical output power for P-doped cascaded Raman fiber lasers was acquired by linear model.
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