搜索

x
中国物理学会期刊

类氖氩46.9 nm和69.8 nm双波长激光最佳参数研究

CSTR: 32037.14.aps.75.20251288

Optimal parameters of Ne-like Ar 46.9 nm and 69.8 nm dual-wavelength laser

CSTR: 32037.14.aps.75.20251288
PDF
HTML
导出引用
  • 采用毛细管放电抽运方案, 获得了类氖氩(Ar8+)离子46.9 nm和69.8 nm双波长激光输出. 在此基础上, 研究了初始氩气气压和主脉冲电流幅值对46.9 nm和69.8 nm激光强度的影响规律. 实验结果表明, 每个主脉冲电流条件下, 都存在最佳的初始气压值, 且69.8 nm激光的最佳气压值低于46.9 nm激光的最佳气压值. 根据最佳气压时的激光强度随主脉冲电流幅值的变化曲线, 46.9 nm和69.8 nm激光的最佳电流值分别为10.9 kA和14.5 kA. 当主脉冲电流幅值为14.5 kA, 初始气压为18.5 Pa时, 可获得46.9 nm和69.8 nm均较强的双波长激光.

     

    Dual-wavelength lasers in the extreme ultraviolet (EUV) band can be utilized in many fields such as high-resolution imaging, EUV nonlinear optics, and high-density plasma diagnostics. In this work, dual-wavelength lasers at 46.9 nm and 69.8 nm from Ne-like Ar (Ar8+) ions pumped by capillary discharge are obtained. In order to change the amplitude of the main pulse current over a wide range, several parameters of the main pulse power supply such as charging voltage of the Marx generator, the conduction voltage of the spark gap switch, and the conductivity of the deionized water in the Blumlein transmission line, are adjusted to vary the amplitude of the main pulse current from 8.4 to15.8 kA. On this basis, the influences of the initial argon pressure and the main pulse current amplitude on the intensities of 46.9 nm and 69.8 nm lasers are studied. The experimental results show that there exists an optimal pressure for each main pulse current amplitude. The optimal pressure for 69.8 nm laser is lower than that for the 46.9 nm laser. Based on the variation of laser intensity with initial pressure and main pulse current amplitude, the optimal experimental parameters for the 46.9 nm laser are a current of 10.9 kA and an initial pressure of 18.1 Pa, and those for the 69.8 nm laser are a current of 14.5 kA and an initial pressure of 18.5 Pa. When the main pulse current amplitude is 14.5 kA and the initial pressure is 18.5 Pa, dual-wavelength lasers at both strong 46.9 nm and 69.8 nm can be generated. The different influencing rules of initial pressure and main pulse current on the 46.9 nm and 69.8 nm lasers can guide other research groups in exploring the possibility of achieving 69.8 nm laser operation by using the existing 46.9 nm laser device. Meanwhile, the research on the optimal parameters of 46.9 nm and 69.8 nm lasers is beneficial for enhancing laser energy and expanding their application fields. One of future studies will focus on the applications of the dual-wavelength laser in the sum frequency and difference frequency of EUV lasers.

     

    目录

    /

    返回文章
    返回