1) Necessary pump
临界泵浦功率
2) Necessary power
临界泵功率
3) pump power
泵浦功率
1.
The influence of the pump power to passive Q-switched period of Nd:YVO4/Cr4+:YAGLaser have been analysed by Theoretical and studied by experimental, then draw a conclusion : the power density is Increasing and the period of Q-switched pulse is becoming short and the account of Q-switched pulse in a pump square wave is increasing following the increase of pump powe
通过对泵浦功率对脉冲LD泵浦Nd:YVO4/Cr4+:YAG激光器被动调Q脉冲周期的影响的理论分析和实验研究,得到如下结论:随着泵浦功率的增加,使得谐振腔内功率密度增加,产生调Q脉冲的周期缩短,一个泵浦方波内调Q脉冲个数不断增加。
2.
On the basis of the rate equation model of the 3-energy-level-system fiber lasers,this paper focuses on the effects of the reflection coefficient of the input mirror R1,the reflection coefficient of the output mirror R2 and the pump power on the optimum length of the cladding fiber lasers L with a numerical emulator,producing a significant result for the study on cladding-pumped fiber lasers.
文章基于三能级系统光纤激光器的速率方程模型,重点分析了输入端反射系数R1、输出端反射系数R2以及泵浦功率这3个因素对包层光纤激光器最佳光纤长度L优化的影响。
3.
Also the relation between the erbiumdoped fiber′s length, pump power, input signal intensity and gain, ASEN of EDFA is given.
阐述了掺铒光纤放大器的放大原理,给出了计算放大器增益和自发辐射噪声的公式,并且给出了增益和噪声与掺铒光纤长度、泵浦功率、输入信号功率之间的关系。
4) Pump lightpower
泵浦光功率
5) critical power
临界功率
1.
Nd:YAG CW laser heat-conduction welding——Ⅱ.calculation of critical power;
Nd:YAG CW激光热传导焊Ⅱ激光热传导焊临界功率的计算
2.
Then the Schrdinger-type nonlinear equation in strong nonlocality was given and from the equation the analytical expressions of the single soliton and the critical power .
得到了非线性系数以及特征长度和预倾角的关系,并且给出了强非局域性的非线性薛定谔方程,最终得到了单孤子和临界功率的解析解。
3.
In experiment,we observe the propagation of solitons in nematic liquid crystals,and determine the critical power of optical spatial solition in different beam width,for example,when the.
实验上,观察了空间光孤子在向列相液晶中的传输,找到了不同束宽下空间光孤子的临界功率。
6) threshold pump power
阈值泵浦功率
1.
For annealed proton exchange Nd∶MgO∶LiNbO 3 waveguide lasers,by assuming Gaussian/Hermite Gaussian and Gaussian/two half Gaussian mode intensity distributions in the direction of width/depth of the waveguide,the threshold pump power and slope efficiencies were calculated and compared with experimental results.
对于Ｎｄ∶ＭｇＯ∶ＬｉＮｂＯ３质子交换波导激光器，通过假设在波导宽度／深度方向上模场强度分布为Ｇａｕｓｓｉａｎ／Ｈｅｒｍｉｔｅ－Ｇａｕｓｓｉａｎ和Ｇａｕｓｓｉａｎ／Ｔｗｏ－ｈａｌｆ－Ｇａｕｓｓｉａｎ两种试探函数，给出了阈值泵浦功率和斜率效率的计算结果。
2.
Starting with rate equation and taking the spatial distributions of pump and laser modes into account,we have derived the general expressions of the threshold pump power and slope efficiency for Nd:MgO:LiNbO 3 and Ti diffused Er:LiNbO 3 waveguide lasers.
本文从速率方程出发，考虑了泵浦光和激光模式的空间分布，分别推导了Ｎｄ：ＭｇＯ：ＬｉＮｂＯ３和钛扩散Ｅｒ：ＬｉＮｂＯ３波导激光器的阈值泵浦功率和斜率效率的一般表达式。
补充资料：泵输出功率
分子式：
CAS号：
性质：又称有效功率或液体功率。单位时间内泵输送出去的液体从泵中获得的有效能量。Pu=ρQgH，式中，Pu为输出功率，W；ρ为液体密度，kg/m3；Q为体积流量，m3/s；H为扬程，m；g为重力加速度，m/s2。
CAS号：
性质：又称有效功率或液体功率。单位时间内泵输送出去的液体从泵中获得的有效能量。Pu=ρQgH，式中，Pu为输出功率，W；ρ为液体密度，kg/m3；Q为体积流量，m3/s；H为扬程，m；g为重力加速度，m/s2。
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