1) UV stimulated emission
紫外受激辐射
2) ultraviolet ampification by stimulated emission of radiation
受激辐射式紫外放大器
3) stimulation radiation
紫区受激辐射
1.
The stimulation radiation of violet region for the atomic sodium and sodium dimer of triplet state were observed.
观察到了由此而产生的分子三重态和原子高位态的紫区受激辐射。
4) ultraviolet stimulated emission
紫外受激发射
1.
ZnO thin films have great potential applications in the fields of ultraviolet detectors, LEDs and LDs thanks to the realization of the optically pumped ultraviolet stimulated emission and self assembled reciprocal stripe.
光泵浦紫外受激发射的获得和自形成谐振腔的发现 ,使ZnO薄膜成为一种备受青睐的新型光电材料 ,在紫外探测器 ,LED ,LD等领域有着广阔的应用前景。
2.
The progress in ultraviolet stimulated emission and p-type doping of ZnO are also discussed.
本文介绍了ZnO薄膜的基本性质以及喷雾热分解、脉冲激光沉积、金属有机物化学气相沉积等制备ZnO薄膜的技术和方法,并着重介绍了在ZnO紫外受激发射和p型掺杂等方面的研究进展。
5) ultraviolet radiation
紫外辐射
1.
The attenuation of ultraviolet radiation in shallow lakes in the middle and lower reaches of Yangtze River;
长江中下游浅水湖泊紫外辐射的衰减
2.
The relations between solar ultraviolet radiation and air pollution in Lanzhou;
兰州城区太阳紫外辐射及其与空气污染的关系
3.
Photoprotective effect of melanin derived from White Silky Fowl on Drosophila melanogaster against ultraviolet radiation;
乌鸡黑色素对果蝇的紫外辐射保护作用
6) ultraviolet irradiation
紫外辐射
1.
Preliminary study on the antiultraviolet irradiation active substances of mycosporine-like amino acids from four kinds of Antarctic ice microalgae;
4种南极冰藻中抗紫外辐射活性化合物类菌胞素类氨基酸(MAAs)的初步研究
2.
The surface modification of ultrahigh-relative molecular weight mass polyethylene(UHMWPE)fiber was conducted via ultraviolet irradiation grafting technology.
采用紫外辐射接枝方法对超高相对分子质量聚乙烯(UHMWPE)纤维表面进行改性。
3.
The space environment effects(including high vacuum、ultraviolet irradiation、cold and thermal cycling)on them were investigated.
通过简单模拟高真空、太阳紫外辐射、冷热交变等空间环境条件,对拟用于飞行器示踪的发光材料SrAl2O4:Eu2+,Dy3+、ZnO:Eu3+,Li1+以及SiO2:Eu3+,Li1+进行了空间环境稳定性试验研究,分别检测了3种材料在高真空条件下的耐强紫外辐射、抗老化、抗热震性能。
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