明亮,高频,圆极化结构阿秒脉冲

A. de las Heras, Nathan J Brooks, Bin Wang, I. Binnie, J. Román, L. Plaja, H. Kapteyn, M. Murnane, C. Hernández-García
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引用次数: 0

摘要

圆偏振(CP)阿秒脉冲的产生要求很高,实现起来也很复杂,特别是在x射线中,标准偏振变换器效率很低。在过去的十年中,高谐波发生器(HHG)的复杂配置为在极紫外波段产生CP高次谐波提供了不同的选择[1],[2]。在这些技术中,只有使用非共线格式[3]才能够在空间上分离具有相同螺旋度的CP高次谐波,从而提供CP阿秒脉冲[4]。该方案基于在驱动激光焦点上沿横向坐标产生一个“旋转偏振光栅”。然而,有效的相互作用区域受到非共线角的限制,进一步限制了整个过程的转换效率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Bright, High-Frequency, Circularly Polarized Structured Attosecond Pulses
The generation of circularly polarized (CP) attosecond pulses is demanding and complicated to achieve, especially in the x-rays where standard polarization converters are highly inefficient. During the last decade, sophisticated configurations of high harmonic generation (HHG) have provided different alternatives to generate CP high-order harmonics in the extreme ultraviolet regime [1], [2]. Among these techniques, only the use of a noncollinear scheme [3] has been able to spatially separate CP high-order harmonics with the same helicity, and thus to provide CP attosecond pulses [4]. Such scheme is based on producing a “rotating polarization grating” along the transverse coordinate across the driving laser focus. However, the efficient interaction region is limited by the noncollinear angle, which further limits the overall conversion efficiency of the process.
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