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基于能量回收直线加速器的全相干光源。

Energy recovery linac based fully coherent light source.

作者信息

Zhao Z T, Wang Z, Feng C, Chen S, Cao L

机构信息

Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai, 201210, China.

University of Chinese Academy of Sciences, Beijing, 100049, China.

出版信息

Sci Rep. 2021 Dec 13;11(1):23875. doi: 10.1038/s41598-021-03354-0.

DOI:10.1038/s41598-021-03354-0
PMID:34903791
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8668884/
Abstract

Energy recovery linac (ERL) holds great promise for generating high repetition-rate and high brightness electron beams. The application of ERL to drive a free-electron laser is currently limited by its low peak current. In this paper, we consider the combination of ERL with the recently proposed angular-dispersion induced microbunching technique to generate fully coherent radiation pulses with high average brightness and tunable pulse length. Start-to-end simulations have been performed based on a low energy ERL (600 MeV) for generating coherent EUV radiation pulses. The results indicate an average brightness over 10 phs/s/mm/mrad/0.1%BW and average power of about 100 W at 13.5 nm or 20 W with the spectral resolution of about 0.5 meV with the proposed technique. Further extension of the proposed scheme to shorter wavelength based on an ERL complex is also discussed.

摘要

能量回收直线加速器(ERL)在产生高重复率和高亮度电子束方面具有巨大潜力。目前,ERL用于驱动自由电子激光器受到其低峰值电流的限制。在本文中,我们考虑将ERL与最近提出的角色散诱导微聚束技术相结合,以产生具有高平均亮度和可调脉冲长度的完全相干辐射脉冲。基于低能量ERL(600 MeV)进行了从头到尾的模拟,以产生相干极紫外(EUV)辐射脉冲。结果表明,采用所提出的技术,在13.5 nm处平均亮度超过10 phs/s/mm/mrad/0.1%BW,平均功率约为100 W;在光谱分辨率约为0.5 meV时平均功率为20 W。还讨论了基于ERL复合体将所提出的方案进一步扩展到更短波长的情况。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/7e80810f4086/41598_2021_3354_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/b5bac159b612/41598_2021_3354_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/f2d702c76b9e/41598_2021_3354_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/9bc3c4784bfe/41598_2021_3354_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/fe463df0590a/41598_2021_3354_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/ceb0220f224b/41598_2021_3354_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/680eb90a0b74/41598_2021_3354_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/245ba155148d/41598_2021_3354_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/2843106b9cfb/41598_2021_3354_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/6ad8310b6c31/41598_2021_3354_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/7e80810f4086/41598_2021_3354_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/b5bac159b612/41598_2021_3354_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/f2d702c76b9e/41598_2021_3354_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/9bc3c4784bfe/41598_2021_3354_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/fe463df0590a/41598_2021_3354_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/ceb0220f224b/41598_2021_3354_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/680eb90a0b74/41598_2021_3354_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/245ba155148d/41598_2021_3354_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/2843106b9cfb/41598_2021_3354_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/6ad8310b6c31/41598_2021_3354_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b34d/8668884/7e80810f4086/41598_2021_3354_Fig10_HTML.jpg

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本文引用的文献

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Momentum dependent [Formula: see text] band splitting in LaFeAsO.LaFeAsO中与动量相关的[公式:见原文]能带分裂。
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A Storage Ring Based Free-Electron Laser for Generating Ultrashort Coherent EUV and X-ray Radiation.基于储存环的自由电子激光,用于产生超短相干极紫外和 X 射线辐射。
稳态微束群聚相干辐射的平均和统计特性。
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