CsLiB6O10真空紫外发生器

N. Umemura, Y. Yap, Y. Mori, T. Sasaki, K. Yoshida, K. Kato
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引用次数: 0

摘要

在之前的出版物1中,我们报道了通过混合Nd:YAG激光在1.0642 μ m的五次谐波和相同Nd:YAG激光的二次谐波泵浦的KTP OPO输出,在CsLiB6O10中产生了低至0.185 μ m的真空紫外(VUV)。然而,没有尝试评估其在波长大于0.19 μ m的材料中产生VUV的性能。作为先前的实验,我们已经证明了在1.0642 μ m的Nd:YAG激光器的五次谐波与同样的Nd:YAG激光器泵浦的H2拉曼振荡器输出之间的2型混合在0.1914 μ m处产生了VUV。表1所示的相位匹配参数是根据文献1中报道的Sellmeier方程和热光学常数计算的。在0.5321 μ m处,将12 mm长的2型二次谐波(SHG)晶体切割为θ≃41°和φ =0°,对晶体的入口表面进行λ /10的抛光处理,并且不进行ar涂层处理。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Vacuum-Ultraviolet Generation in CsLiB6O10
In previous publication 1 , we have reported the vacuum-ultraviolet (VUV) generation down to 0.185 μ m in CsLiB6O10 by mixing the fifth harmonic of a Nd:YAG laser at 1.0642 μ m and the output of a KTP OPO pumped by the second-harmonic of the same Nd: YAG laser. However, no attempt was made to evaluate its performance for VUV generation at wavelengths longer than 0.19 μ m in this material. As a prior experiment, we have demonstrated the VUV generation at 0.1914 μ m by type-2 mixing between the fifth harmonic of a Nd:YAG laser at 1.0642 μ m and the output of a H2 Raman oscillator pumped by the same Nd:YAG laser. The phase-matching parameters tabulated in Table 1 were calculated with the Sellmeier’s equations and thermooptic constants reported in Ref.1. The 12-mm-long crystal used in this experiment was cut at θ ≃ 41 ° and ϕ =0 ° for type-2 second harmonic generation (SHG) at 0.5321 μ m. The entrance faces were polished with a flatness of λ /10 and no AR-coatings are applied for this crystal.
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