由100千赫薄板激光系统产生的皮秒深紫外脉冲

H. Turčičova, O. Novák, L. Roškot, J. Mužík, M. Smrž, A. Endo, T. Mocek
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引用次数: 3

摘要

我们报道了515 nm的皮秒脉冲和257 nm和206 nm的深紫外脉冲的产生。它们是在1030nm基波长高功率二极管泵浦Yb:YAG薄板激光器的第二、四、五次谐波频率下产生的。基波长的激光是基于薄板作为有源介质的两级再生放大器中振荡脉冲的啁啾脉冲放大。在零声子线处使用二极管泵浦。脉冲的重复频率为~100 kHz,脉冲持续时间为2-10 ps,脉冲能量≤2 mJ。基束在LBO晶体中以42%的效率加倍。随后,在CLBO晶体中通过倍频的二次谐波频率产生第四次谐波频率(257 nm)。基束经过SHG后的未转换部分与四次谐波束作为1ω+4ω的频率和在另一个CLBO晶体中产生五次谐波频率(206nm)。在有效的光转换中有两个重要的问题:主要由双光子吸收(TPA)引起的非线性吸收和相互作用脉冲的适当定时。在我们的模拟中,我们考虑了TPA,并研究了在产生五次谐波时,1ω和4ω脉冲的不同时序对CLBO的影响。结果发现,要获得最高的5ω输出,需要在4ω脉冲后的1ω脉冲延迟1.4 ps。5ω脉冲持续时间也受定时的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Picosecond deep ultraviolet pulses generated by a 100 kHz thin-disk laser system
We report on the generation of picosecond pulses at 515 nm and deep ultraviolet pulses at 257 nm and 206 nm. They are generated as second, fourth and fifth harmonic frequencies of the high power diode-pumped Yb:YAG thin-disk laser at the fundamental wavelength of 1030 nm. The laser at the fundamental wavelength is based on a chirped-pulse amplification of oscillator pulses in two-stage regenerative amplifier based on thin-disks as active media. The diode pumping at the zero phonon line is used. The pulses are produced at ~100 kHz repetition frequency, 2-10 ps pulse duration and ≤2 mJ pulse energy. The fundamental beam is doubled in an LBO crystal at an efficiency of 42%. Subsequently the fourth harmonic frequency (257 nm) is produced by frequency doubling of the second harmonic frequency in a CLBO crystal. The unconverted part of the fundamental beam after SHG is used with the fourth harmonic beam as 1ω+4ω frequency sum in a further CLBO crystal for the fifth harmonic frequency (206 nm) generation. Two issues are important in the efficient optical conversion: nonlinear absorption given mainly by two-photon absorption (TPA) and proper timing of interacting pulses. In our simulations we take into account TPA and study the consequences of different timing of 1ω- and 4ω-pulses on the CLBO when generating the 5th harmonic. It was found that 1.4 ps delay of the 1ω-pulse after the 4ω-pulse is necessary to get the highest 5ω-output. Also the 5ω-pulse duration is affected by the timing.
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