Stimulated Raman emission at 8·84 μm

M. Martín, E. Thomas
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引用次数: 3

Abstract

Focusing the output of a Q-switched ND3+: glass laser (frequency 9441 cm-1) into a high-pressure hydrogen cell (hydrogen molecular vibration frequency 4155 cm-1) produces second Stokes stimulated Raman emission at 9441 - (2 × 4155) = 1131 cm-1 or 884 μm. The dependence of this emission on hydrogen pressure has been investigated, the maximum power of 180 w being reached when the gas pressure was 250 lb in-2, the laser power 30 MW, and the first Stokes power (at 189 μm) 2 MW. At laser powers above 30 MW evidence for plasma formation is presented, and this is put forward as the reason why the output at 884 μm cannot be increased beyond 180 w.
在8·84 μm处受激拉曼辐射
将调q ND3+:玻璃激光器(频率为9441 cm-1)的输出聚焦到高压氢电池(氢分子振动频率为4155 cm-1)中,产生第二次斯托克斯激发拉曼辐射,波长为9441 - (2 × 4155) = 1131 cm-1或884 μm。实验结果表明,当气体压力为250 lb / 2时,激光功率为30 MW,第一Stokes功率(189 μm)为2 MW,最大功率为180 w。在激光功率大于30 MW时,等离子体形成的证据被提出,这是为什么884 μm的输出不能增加到180 w以上的原因。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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