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两种透射率入射腔镜对894.6nm倍频腔转换效率的比较

Comparison of the conversion efficiency of 894.6nm frequency doubling cavity with different transmission input coupler

  • 摘要: 为了在对基频光透射率分别为5%和10%的两种入射腔镜(其它参数相同)中择优, 利用波长对应于铯原子D1线的894.6nm半导体激光作为基频光, 抽运以周期极化磷酸氧钛钾(PPKTP)晶体作为非线性介质的两镜驻波倍频腔, 通过外腔倍频过程产生447.3nm蓝光, 对利用这两种腔镜搭建倍频腔所产生的蓝光进行了对比。结果表明, 在注入350mW基频光、倍频腔采用透射率为5%的入射腔镜时, 制备了178mW蓝光, 倍频效率为50.8%, 0.5h功率起伏为1.4%;采用10%透射率腔镜的倍频腔获得131mW蓝光, 倍频效率为37.4%, 0.5h功率起伏为0.7%;使用5%透射率入射腔镜的倍频效果更好。该研究对产生铯原子D1线非经典光场所需高质量抽运源的制备具有重要指导意义。

     

    Abstract: In order to choose a better input coupler, the conversion efficiency of the frequency doubling cavity were studied in the case of the transmittance of the input coupler to the fundamental light of 5% and 10%, respectively. 447.3nm blue light was obtained by external-cavity frequency doubling of a tapered amplifier-boosted continuous-wave diode laser at cesium D1 line. The frequency doubling cavity consists of a two-mirror standing wave cavity with a periodically poled KTiOPO4 (PPKTP) crystal inside. With a maximum fundamental power around 350mW, the frequency doubling cavity with a 5% transmittance input coupler generate 178mW blue light, corresponding to a conversion efficiency of 50.8%. With the input coupler with a 10% transmittance at the fundamental wavelength, 131mW of blue light is obtained, and the corresponding conversion efficiency is 37.4%. With a maximum input fundamental power, the output blue power was measured for 0.5h. In the frequency doubling cavity with 5% transmittance input coupler, the root mean square fluctuation is 1.4%, while the other is 0.7%. The result shows that the input coupler with 5% transmittance is better. This research is helpful for preparing high quality pump light resources to generate nonclassical light at cesium D1 line.

     

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