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output mirror
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  输出镜
     Maximum laser output power of 900 mw was obtained with a discharge current of 100 A and a discharge voltage of 260 V, the pressure at 16m bars(Ne:Ar= 1000:1), the transmissivity of the coupling output mirror at 3.6% and the reflectivity of mirror at 99.2%.
     当放电电流为100安、放电电压为260伏、充气压力为16毫巴(Ne:Ar=1000:1)、耦合输出镜透射率为3.6%、全反射镜的反射率为99.2%时,获得最大紫外激光输出为900毫瓦.
短句来源
     Study of output mirror of waveguide CO2 laser
     波导CO_2激光器输出镜的研究
短句来源
     In the experiment,A set of Ti:sapphire resonator mirrors from 750 to 850 nm is chosen,and the transmission rate of the output mirror is 5%,10%,15% respectively.
     实验中,选择750~850nm宽带膜片组,钛宝石输出镜的透过率分别为T=5%、10%和15%。
短句来源
     In the experiment,the transmission rate of the output mirror of (10%,30%,35%,40%) are chosen respectively,and the maximum(512 W) output power at1 064 nm with 32% optical-optical conversion efficiency is achieved.
     在实验中,1 064 NM输出镜的透过率分别为T=10%、30%、35%和40%,得到了512 W 1 064 NM输出,光-光转换效率达到32%。
短句来源
     At the repetition rate of 4kHz,output mirror transmission of 30%,input current of 14.5A,the KTA OPO generated the highest average output power of 613.4mW at1.57μm with pulse width of 2.5ns and the peak power of 61kW.
     当声光重复频率为4kHz,输出镜透过率为30%,泵浦电流为14.5A时,波长为1.57μm,KTA晶体参量激光平均输出功率最大为613.4mW,脉冲宽度约2.5ns,峰值功率超过61kW。
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  输出反射镜
     The results show that the single-mode operation with high slope efficiency, low threshold and high output power can be achieved in waveguide laser with short and heavily doped waveguide and optimized reflectivity of output mirror.
     理论分析的结果表明用长度较短的重掺杂波导并优化激光器的输出反射镜的反射率时,可以获得较高的功率输出和斜率效率,其抽运阈值也较低。
短句来源
     For the vicinity of threshold value conditions,the optimum reflectivity of the output mirror which makes the laser reach the maximum output power is about 0.4~0.7.For strong pumping conditions,the smaller the reflectivity of the output mirror is,the higher the output power is.
     在近阈值情况下进行泵浦,输出耦合镜有一个最佳反射率,使输出功率达到最大。 一般反射率应取在0.4~0.7之间,但在强泵浦情况下,输出反射镜的反射率越低越好。
短句来源
     The simulation and analysis are carried out by using a numerical method. On the basis of the above simulation and analysis,the influence of fiber length,output mirror relectivity,pump power and etc on the output power and thrshold are analyzed and compared.
     利用数值方法进行了模拟分析,在此基础上,分析比较了光纤长度、输出反射镜反射率、泵浦功率等因素对输出功率和阈值的影响。
短句来源
  “output mirror”译为未确定词的双语例句
     When the reflectivity of output mirror varies from 0. 80 to 0. 95,the output coupling has no great effect on output efficiency.
     在反射率为0.80~0.95之间,输出耦合对输出效率影响不明显。
短句来源
     Without any dispersion elements in cavity, 6.44 W of Ti: sapphire laser output is obtained when the pump power is 16 W and the transmissivity of output mirror is 30%, the optical-to-optical conversion efficiency is higher than 40%.
     自由运转时,在抽运光功率为16 W,透过率为30%时,获得了最高6.44 W的掺钛蓝宝石激光输出,相应光光转换效率大于40%。
短句来源
     Consequently, using a plane-concave cavity, the output mirror coupler with 1.5% transmission at 1123-nm and having a high transmission (>80%) in the 1064-nm region, when the pumping power is 1.37W, a laser output power of 119mW and optical-optical conversion efficiency of 8.7% are attained.
     1064nm的透过率大于80%。 当入射进YAG晶体内的泵浦光功率为1.37W时,我们获得了119mW的1123nm激光输出,光-光转换效率为8.7%。
     When the transmission of the output mirror is 15 %,the threshold is 0.251 W. When the pump power is 21 W,the output power of the cw laser at 1.06 μm is 10.52 W,corresponding to an optical to optical efficiency of 50 %.
     当输出窗片透射率为15 %时 ,阈值为 0 .2 5 1W,对应着 2 1W的泵浦功率 ,得到 10 .5 2 W的 1.0 6μm连续光输出 ,光 -光转换效率达到 5 0 %。
短句来源
     The laser cavity is a plane concave cavity. The output mirror curvature radius is 1m and transmissivity T is 0.33. By KD ★ P Q switch,the laser pulse duration is 12.7ns and single pulse energy is 1.97mJ. Optical beam quality M 2 x =2.69 and M 2 y =1.87.Its repetition rate is 98Hz.
     用 KD★ P电光 Q开关 ,得到输出脉宽为 12 .7ns、单脉冲能量 1.97m J的激光 ,光束质量 M2x=2 .6 9、M2y=1.87,重复频率 98Hz
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  output mirror
Its dependence on the output mirror reflectivity and residual ground-state absorption in the emission region is analysed.
      
The possibility of controlling the directionality of radiation depending on the spectral and angular characteristics of the output mirror is shown.
      
In the laser of the second type the role of the output mirror was played by a loop-shaped fiber-optic reflector made on the basis of a V-shaped fused three-fiber splitter.
      
Such output mirror possesses good separation of the pump (λ≈10μm) and FIR radiation without losses.
      
Design of a low-power tunable quasioptical gyrotron with a slotted output mirror
      
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Experimental results of an investigation on a 1.2-meter slotted UV-Cu+-laser in Optisches der Technische Universitat, Berlin, Germany are given. The experimenting device used was a hollow cathode with a discharge length of 1.2 meters and a slot cross-section of 2x6 mm. Maximum laser output power of 900 mw was obtained with a discharge current of 100 A and a discharge voltage of 260 V, the pressure at 16m bars(Ne:Ar= 1000:1), the transmissivity of the coupling output mirror at 3.6% and the reflectivity...

Experimental results of an investigation on a 1.2-meter slotted UV-Cu+-laser in Optisches der Technische Universitat, Berlin, Germany are given. The experimenting device used was a hollow cathode with a discharge length of 1.2 meters and a slot cross-section of 2x6 mm. Maximum laser output power of 900 mw was obtained with a discharge current of 100 A and a discharge voltage of 260 V, the pressure at 16m bars(Ne:Ar= 1000:1), the transmissivity of the coupling output mirror at 3.6% and the reflectivity of mirror at 99.2%. The single pass gain of the laser has been estimated at 5.8% per meter.

本文报导了“1.2米槽型紫外铜离子激光器”的实验结果.实验装置的中空阴极放电长度为1.2米、槽切面为2×6毫米.当放电电流为100安、放电电压为260伏、充气压力为16毫巴(Ne:Ar=1000:1)、耦合输出镜透射率为3.6%、全反射镜的反射率为99.2%时,获得最大紫外激光输出为900毫瓦.激光系统的增益系数为每米5.8%.

The laser intra-cavity absorption method is of a newly developed technique used for the determination of weakly absorbed substance, it has the merits of high sensitivity and simple operation. This paper has, studied the effects of various laser parameters(including resonant cavity length, pump energy, the transmittance of output mirror, pulse repetition frequency, etc.) on sensitivity. A preliminary theoretical exploration is presented. An important reason why the formula proposed by Horlick does not coincide...

The laser intra-cavity absorption method is of a newly developed technique used for the determination of weakly absorbed substance, it has the merits of high sensitivity and simple operation. This paper has, studied the effects of various laser parameters(including resonant cavity length, pump energy, the transmittance of output mirror, pulse repetition frequency, etc.) on sensitivity. A preliminary theoretical exploration is presented. An important reason why the formula proposed by Horlick does not coincide with the result of this experiment is due to the fact that two reflective mirrors of the resonant cavity can not be strictly parallel. The corresponding formula is deduced.Experimental results showedn that Beer's law is obeyed in the range of Neodymium ion concentration of 2 ×10-3-1×10-2 M, the sensitivity increases by a factor of 27, as compared with that of the conventional absorption spectrometry, some rare-earth elements like La, Ce, Pr, Sm, Y etc. do not interfere. This method can be used for the determination of Neodymium in light rare-earth mixtures.

本文通过钕的激光内腔吸收的测定,研究了激光器的各种参数(包括谐振腔长、泵浦能量、反射镜间的平行度、输出反射镜的透光率和脉冲重复率等)对激光内腔吸收法灵敏度的影响,并在理论上进行了初步的探讨。 实验结果表明,本法灵敏、快速。钕离子的检定限可达1×10~(-3)M,比常用的外腔吸收光度法灵敏度提高27倍。本法可用于轻稀土混合物中钕的定量测定。

In this paper the complete compensation condition of astigmatism for the folded 3-mirror laser resonant cavity, whose output mirror is a plane mirror, is given. It is also proved that the astigmatic compensation conditions, appeared in some of the papers previously...such as in references [1] and [5], are just the kinds of approximation. In this paper a method of adjusting this sort of cavity is also worked out.

本文给出了当输出镜是平面镜时激光三镜折叠谐振腔象散完全补偿的条件,以及证明了以前出现在另一些文献中——如本文的参考文献[1]、[5]——的象散补偿条件的近似性。本文同时也给出了这种腔的调试方法。

 
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