1) Stimulated Raman pumping
受激Raman泵浦
2) stimulated Raman emissin
受激Raman发射
3) SRS
受激Raman散射
1.
Two kinds of self-pulsation are observed in the fiber laser with a low Q cavity, one is the pulse generated from passive Q-switching of saturable absorption; the other is the giant pulse due to stimulated Raman scattering (SRS) in the fiber.
发现低Q值腔光纤激光器具有两种形式的自脉动输出,一种是饱和吸收被动调Q产生的自脉冲,另一种是与光纤中的受激Raman散射(SRS)效应相对应的阵发性巨脉冲。
4) stimulated Raman scattering
受激Raman散射
1.
Stimulated Raman scattering from interaction of 2ns,351nm laser with hohlraum;
2ns,351nm激光黑腔靶受激Raman散射实验研究
2.
Stimulated Raman scattering from holraum irradiated with 351nm laser light;
351nm激光入射大腔靶的受激Raman散射光谱
3.
The effect of collision on stimulated Raman scattering;
碰撞对受激Raman散射的影响
5) Stimulated Raman specta
受激Raman光谱
6) laser pumping
激光泵浦
1.
In a beam-gas cell arrangement the absolute cross sections for the reactions of metastable Xe(3P0) and Xe(3P2) atoms with N2 were measured by means of a pulsed laser pumping technique.
在束-气池构型下用脉冲激光泵浦技术测量了亚稳态Xe(~3P_0)和Xe(~3P_2)与N_2传能生成N_2(B,v)的绝对截面。
补充资料：受激激辐射跃迁概率
分子式：
CAS号：
性质：处于激发态的原子Nj，受能量的hv(h为普朗克常数)的入射光子的激励下，从激发态跃迁到低能级。当在dt时间内，在dNjo个激发态原子发生受激辐射，则dNjo与跃迁前高能级上的原子数Nj，辐射能量密度ρ（v），激发时间dt成正比，即dNjo=BjoNjρ(v)dt。式中Bjo为受激跃迁系数。Bjo与ρ(v)的乘积称受激辐射跃迁概率，定义为
CAS号：
性质：处于激发态的原子Nj，受能量的hv(h为普朗克常数)的入射光子的激励下，从激发态跃迁到低能级。当在dt时间内，在dNjo个激发态原子发生受激辐射，则dNjo与跃迁前高能级上的原子数Nj，辐射能量密度ρ（v），激发时间dt成正比，即dNjo=BjoNjρ(v)dt。式中Bjo为受激跃迁系数。Bjo与ρ(v)的乘积称受激辐射跃迁概率，定义为
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