Zhao Yongpeng, Liu Tao, Zhang Wenhong, Li Wei, Cui Huaiyu
Opt Lett. 2016 Aug 15;41(16):3779-82. doi: 10.1364/OL.41.003779.
With a 45-cm-long capillary, we obtained a saturated 69.8 nm laser with a gain coefficient of 0.4 cm and a gain length product of 18. In order to increase the laser energy further, a double-pass amplification of the 69.8 nm laser was first realized with a SiC mirror without a coating. With a half cavity, the effective plasma column length and the effective gain length product can reach 84 cm and 33.7, respectively. The amplitude of a laser pulse for double-pass amplification is 9 times larger than that for single-pass amplification. In addition, the full width at half-maximum (FWHM) pulse width of a laser pulse and FWHM divergence for single-pass amplification are 1.4 ns and 0.5 mrad, respectively, which increase to 2.2 ns and 3.4 mrad for double-pass amplification.
使用一根45厘米长的毛细管,我们获得了饱和的69.8纳米激光,其增益系数为0.4厘米,增益长度乘积为18。为了进一步提高激光能量,首先使用未镀膜的碳化硅镜实现了69.8纳米激光的双程放大。在半腔情况下,有效等离子体柱长度和有效增益长度乘积分别可达84厘米和33.7。双程放大的激光脉冲幅度比单程放大的大9倍。此外,单程放大的激光脉冲的半高全宽(FWHM)脉冲宽度和FWHM发散角分别为1.4纳秒和0.5毫弧度,双程放大时分别增加到2.2纳秒和3.4毫弧度。