Improvement of pulsed optical parametric oscillator by spatio-temporal shaping of the pump beam

A. Mugnier, V. Kermene, A. Barthélémy
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Abstract

Summary form only. During the past years high-energy, nanosecond OPOs have been the subject of numerous investigations because of their potential applications as powerful tunable sources. However, they require short cavity length to achieve high conversion efficiency and large pump cross-section to avoid optical damages. Typical cavities correspond to high Fresnel number and produce beams of bad spatial quality. An increase in OPO output energy frequently leads to a reduction in OPO brightness. We propose a new method based on spatio-temporal shaping of the pump wave to improve the transverse properties of OPO emission at high energy level. Extracavity optical parametric generation is usually performed in two steps (at least). The pump pulse is split in two parts of unequal intensity. The weakest pulse, once confined in a tightly focused beam serves for the actual OPG, while the pulse of high energy is used for amplification during a second pass through the nonlinear crystal. This permits most of the times to preserve a good beam profile. The same idea has been applied to OPO. At the beginning of the pumping the pump beam size is chosen to be small enough to ensure a transverse single mode oscillation in the cavity and energetic enough to start the oscillation. Then the following part of the pump beam, bringing the main part of the energy, is spread on a larger cross section to amplify the oscillating wave.
利用抽运光束的时空整形改进脉冲光参量振荡器
只有摘要形式。在过去的几年里,由于其作为强大的可调谐源的潜在应用,高能纳秒opo已经成为许多研究的主题。但它们需要较短的腔长以获得较高的转换效率,需要较大的泵浦截面以避免光学损伤。典型的空腔对应高菲涅耳数,产生空间质量差的光束。OPO输出能量的增加经常导致OPO亮度的降低。本文提出了一种基于抽运波时空整形的新方法来改善OPO高能量发射的横向特性。外腔光参量的生成通常分两步(至少)进行。泵浦脉冲被分成强度不等的两部分。最弱的脉冲,一旦被限制在紧密聚焦的光束中,用于实际的OPG,而高能量脉冲用于在第二次通过非线性晶体时进行放大。这允许在大多数情况下保持良好的光束轮廓。同样的想法也适用于OPO。在抽运开始时,选择足够小的抽运光束尺寸,以确保腔内的横向单模振荡和足够的能量来启动振荡。然后,带着主要能量的泵浦光束的下一部分在更大的横截面上扩散,以放大振荡波。
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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