1) Coherent Anti-Stokes Raman Scattering
相干反Stokes Raman散射
1.
The work in this dissertation is mainly about techniques and applications of PARS (Photoacoustic Raman Spectroscopy) and RIKE (Raman Induced Kerr Effect), and also concerning on techniques of SRGS (Stimulated Raman Gain Spectroscopy) and CARS (Coherent Anti-Stokes Raman Scattering).
论文的主要工作是关于Raman光声光谱(Photoacoustic Raman Spectroscopy，PARS)技术和与Raman共振相关的四波混频——Raman诱导Kerr效应偏振光谱(Raman Induced Kerr Effect，RIKE)技术及其应用所进行的研究；同时也涉及受激Raman增益光谱(Stimulated Raman Gain Spectroscopy，SRGS)和相干反Stokes Raman散射(Coherent Anti-Stokes Raman Scattering，CARS)光谱技术的少量工作。
2) Reverse Stokes Raman scattering
反Stokes Raman背向散射
3) Raman scattering
Raman散射
1.
Micro-Raman scattering study of hexagonal InGaN epitaxial layer;
六方相InGaN外延膜的显微Raman散射
2.
Design of distributed optical fiber temperature sensing system based on spontaneous Raman scattering;
基于自发Raman散射分布式光纤测温系统设计
3.
The optimization design of Raman scattering line-type optical fiber temperature detector
Raman散射线型光纤感温火灾探测器的优化设计
5) Raman scattering spectra
Raman散射光谱
1.
Raman scattering spectra under low temperature of several typical Cd_(0.96) Zn_(0.04) Te surfaces;
用低温Raman散射光谱研究不同处理的CdZnTe表面
6) raman scattering
拉曼(Raman)散射
补充资料：相干散射和非相干散射
再辐射的光量子频率和被吸收的光量子频率准确相等的散射过程称为相干散射。在相干散射的情况下，源函数准确地等于平均辐射强度。再辐射的光量子频率和被吸收的光量子频率不相等的散射过程称为非相干散射。在天体物理中，存在一系列因素使散射过程成为非相干散射。主要的因素是：原子的能级有一定的宽度、原子的热运动和湍动以及压力效应等。对于非相干散射，源函数是相当复杂的。
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