离子通道激光器的实验机会

M. Litos, R. Ariniello, C. Doss, K. Hunt-Stone, J. Cary
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引用次数: 2

摘要

离子通道激光器(ICL)最初是作为一种紧凑的、基于等离子体的自由电子激光器(FEL)替代品而提出的[1]。在许多方面,它与FEL类似,尽管它本身也有一些明显的优势。最值得注意的是,ICL可以容纳更大的电子能量扩散,使其更适合高亮度等离子体注入光束。此外,相同的辐射体(等离子体源)可以用来产生椭圆偏振光而不改变,这是自由电子激光器所没有的特征。从历史上看,电子束质量和等离子体源的发展不足以证明ICL。此外,由于ICL产生的辐射固有的短瑞利长度,它显得不利。然而,最近的文献表明,尽管瑞利长度很短,但可以实现高增益[2]。此外,目前和不久的将来的设施能够为ICL提供适当的光束和等离子体源。介绍了在先进加速器实验测试II设施(FACET-II)演示ICL的实验机会,利用来自SLAC国家加速器实验室直线加速器的10 GeV光束和1 GeV高亮度等离子体注入光束。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Experimental Opportunities for the Ion Channel Laser
The ion channel laser (ICL) was originally proposed as a compact, plasma-based alternative to the free electron laser (FEL) [1]. It is, in many ways, analogous to the FEL, though it offers some distinct advantages all on its own. Most notably, the ICL can accommodate a larger electron energy spread, making it better suited for high-brightness plasma-injected beams. In addition, the same radiator (plasma source) can be used to produce elliptically polarized light without alteration, a feature that is absent in an FEL. Historically, electron beam quality and plasma source development were insufficient for the demonstration of the ICL. In addition, the ICL appeared unfavorable due to the inherently short Rayleigh length of the radiation it produced. Recent literature, however, has shown that high gain can be achieved, despite the short Rayleigh length [2]. In addition, current and near-future facilities are able to provide appropriate beams and plasma sources for the ICL. Experimental opportunities to demonstrate an ICL at the Facility for Advanced Accelerator Experimental Tests II (FACET-II) are presented, utilizing both a 10 GeV beam originating from the SLAC National Accelerator Laboratory linac, and a 1 GeV high-brightness, plasma-injected beam.
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