1) emission cross section
发射截面
1.
It is found that the peak stimulated emission cross section of EDTNb g.
53μm处的受激发射截面提高8%,其峰值达8。
2.
It was found that the peak stimulated emission cross section of EDTNb glasses was 8.
53μm处的受激发射截面提高了8%,其峰值达8。
3.
Based on Yb 3+ doped laser glass reported abroad, the Yb 3+ doped glasses with higher emission cross section are obtained experimentally.
在国外报道的一些掺镱 (Yb3 + )激光玻璃基础上 ,实验研究得到发射截面更大的掺 Yb3 +玻璃。
2) emission cross-section
发射截面
1.
The emission cross-section at 1040 nm is 0.
51×10-20cm2,在1040nm处的发射截面为0。
2.
According to McCumber theory,the absorption and stimulated emission cross-sections corresponding to the 3H6←→3F4 transitions of Tm3+(at 1.
0μm)跃迁的吸收截面和受激发射截面。
3.
Meanwhile,according to McCumber theory,the absorption and emission cross-sections corresponding to the 3F4→3H6 transitions of Tm3+ at 1.
8μm)跃迁的吸收截面和受激发射截面,该荧光的受激发射截面峰值比氟锆铝酸盐玻璃大。
3) stimulated-emission cross-section
受激发射截面
1.
The calculation of stimulated-emission cross-section and the testing of fluorescence lifetime of Nd∶GGG crystal;
Nd∶GGG晶体荧光寿命的测试及受激发射截面的计算
2.
The integrated absorption cross-sections at 810 nm and the stimulated-emission cross-sections at 1.
06μm处的受激发射截面都是最大的。
4) Stimulated emission cross section
受激发射截面
1.
Techniques for measuring the polarized absorption spectrum,polarized stimulated emission cross section and fluorescent lifetime of Nd:YAP crystal are fully discussed.
从分析Nd:YAP和Nd:YAG两种激光晶体的优缺点入手,指出前者的各向异性能够提供许多特殊的用途,讨论了它的能级和光谱特性,详细介绍了该晶体偏振吸收谱、偏振受激发射截面谱和荧光寿命的测量方法,并给出了两块沿a轴切割的Nd:YAP晶体的测量结果和分析。
2.
The description about the effective stimulated emission cross section of R_2→Y_3 transition of Nd∶YAG crystal in the book "Solid-State Laser Emgineering"written by W.
Koechner先生所著的《Solid-StateLaserEngineering》一书中关于Nd∶YAG晶体R2→Y3跃迁有效受激发射截面的描述进行讨论。
3.
By using the experimentally measured threshold data and slope efficiency, the stimulated emission cross section of Nd∶GdVO 4 crystal was determined to be 1.
利用实验测得的阈值抽运功率和斜率效率 ,计算了Nd∶GdVO4晶体在 1 34μm波长处的受激发射截
5) stimulated emission cross-section
受激发射截面
1.
The radiative transition probabilities(A)and the stimulated emission cross-sections(σ_e)of Eu~ 3+ ion between ~5D_0 and ~7F_J(J=1,2,4)are obtained.
从发射光谱出发获得了Eu3+光学跃迁的J-O参数Ω2、Ω4,并计算了Eu3+离子5D0→7FJ(J=1,2,4)的自发辐射跃迁几率A以及受激发射截面σp。
6) stimulated emission cross sections
受激发射截面
1.
The stimulated emission cross sections of Er3+in tellurite glass was calculated,σemi = 9.
应用MeCumber理论计算了Er3+在碲酸盐玻璃中的受激发射截面σemi=9。
补充资料：导弹机动发射(见导弹发射方式)
导弹机动发射(见导弹发射方式)
maneuverable launching of missile
算薰;笙簌巍骂 able launching 式。
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