全光汤姆孙散射

闫文超; 朱常青; 王进光; 冯杰; 李毅飞; 谭军豪; 陈黎明

doi:10.7498/aps.70.20210319

摘要

随着激光和加速器技术的发展, 激光场强度和粒子能量也有所提升, 在高场强和高电子能量的条件下, 电子与光子的汤姆孙散射过程将达到高度非线性状态, 在这种状态下会发生多光子效应, 即单个电子同时与多个光子相互作用并辐射一个高能光子, 此过程通常称为多光子汤姆孙散射. 当场强和粒子能量变得更高时, 需要引入量子电动力学理论来解决极端光场物理中的动理学过程. 近期, 全球多台数拍瓦激光装置逐渐投入使用, 激光等离子体相互作用中的此类效应会变得极其显著. 而全光汤姆孙散射成为目前研究极端光场物理最佳的实验方案, 因此, 系统地研究全光多光子汤姆孙散射是本领域未来十年极其重要的方向. 本文对近年来全光汤姆孙散射实验从单光子、低阶多光子到高阶多光子的研究进展进行了综述, 并对其未来的发展方向进行了展望. 另外, 伴随着散射过程产生的准直高亮X/伽马射线, 有望发展成为具有重要应用价值的紧凑型超亮高能光源.

关键词:

Abstract

With the development of laser and accelerator technology, and improvement of the particle energy and field intensity, the scattering process between electron and photon will reach the highly nonlinear regime, where the multi-photon process takes place and the quantum electrodynamics starts to play a role. In the near future, with the commissioning of the multi-PW laser facilities, these effects will be available. In this article, we review the recent progress of electron-photon scattering experiments, from single or few-photon regime to high-order multi-photon regime. In the scattering process, collimated bright X/gamma-energy photons are generated, making it possible to realize a compact top-table bright light source, which is also known as inverse Compton scattering source. Finally, the prospects and challenges of scattering experiments are discussed.

Keywords:

作者及机构信息

1.
上海交通大学物理与天文学院, 激光等离子体教育部重点实验室, 上海　200240

2.
上海交通大学IFSA协同创新中心, 上海　200240

3.
中国科学院物理研究所, 光物理重点实验室, 北京　100190

4.
中国科学院大学物理学院，北京　100049

通信作者: 闫文超, wenchaoyan@sjtu.edu.cn ; 陈黎明, lmchen@sjtu.edu.cn

基金项目: 国家自然科学基金(批准号: 11991073, 12074251, 11905289, 11805266)、中国工程物理研究院挑战计划(批准号: TZ2018005)、国家重点基础研究发展计划(批准号: 2017YFA0403301)和中国科学院先导专项(批准号: XDA25030400, XDB17030500)资助的课题

Authors and contacts

1.
Key Laboratory for Laser Plasmas, Ministry of Education, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China

2.
Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University, Shanghai 200240, China

3.
Key Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China

4.
School of Physical Sciences, University of Chinese Academy of Scineces, Beijing 100049, China

Corresponding author: Yan Wen-Chao, wenchaoyan@sjtu.edu.cn ; Chen Li-Ming, lmchen@sjtu.edu.cn

Funds: Project supported by the National Natural Science Foundation of China (Grant Nos. 11991073, 12074251, 11905289, 11805266), the Science Challenge Project of China Academy of Engineering Physics (Grant No. TZ2018005), the National Basic Research Program of China (Grant No. 2017YFA0403301), and the Strategic Priority Research Program of the Chinese Academy of Sciences (Grant Nos. XDA25030400, XDB17030500)

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参考文献

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施引文献

图 1 近期国际上全光汤姆孙散射的主要实验进展及发展方向

Fig. 1. Recent progress and road map of the Thomson scattering.

下载: 全尺寸图片幻灯片

图 2 两种不同的实验方案　(a)单束激光-等离子体镜方案; (b)双光束方案

Fig. 2. Two different experimental geometries for all-optical scattering: (a) Single beam plasma mirror regime; (b) dual beam regime.

下载: 全尺寸图片幻灯片

图 3 等离子体镜方案产生X射线的示意图

Fig. 3. Illustration of the X-ray generation via plasma mirror regime.

下载: 全尺寸图片幻灯片

图 4 全光逆康普顿散射X射线随电子能量的定标率, 红色代表使用800 nm散射激光, 蓝色代表使用400 nm散射激光

Fig. 4. Scaling law of inverse Compton scattering X-ray energy by fundamental and second-order harmonics of Ti: Sapphire scattering laser.

下载: 全尺寸图片幻灯片

图 5 文献[91]报道的全光汤姆孙散射的非线性效应, a₀明显影响了X射线能量的定标率

Fig. 5. Scaling shift in the few-photon scattering experiment. Reprinted with permission from Ref. [91].

下载: 全尺寸图片幻灯片

图 6 文献[35]报道的高阶多光子效应

Fig. 6. Effect of high-order multi-photon scattering reported in Ref. [35].

下载: 全尺寸图片幻灯片

图 7 汤姆孙散射截面随a₀变化的定标率, 该变化曲线由文献[60]的理论计算得出

Fig. 7. Scaling law of the Thomson scattering cross section vs. a₀ in the rest frame. The blue range means where the RR effect matters. The curves were plotted based on Ref. [60]

下载: 全尺寸图片幻灯片

表 1 常见全光逆康普顿X射线源参数

Table 1. Parameter of all-optical inverse Compton scattering X-ray source.

参数	数值
源尺寸/μm	～5 (root mean square)
发散角/ mrad	～5 (FWHM)
峰值能量	keV—20 MeV
单能性	准单能(线性)/连续谱(非线性)*
单发光子数	10⁷—10¹⁰
峰值亮度/ ph·(s·mm²·mrad²·0.1%BW)^–1	10¹⁷—10²²

下载: 导出CSV

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[2]	Barkla C G 1903 Proc. Phys. Soc. London 19 185 Google Scholar
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[4]	Stephenson R J 1967 Am. J. Phys. 35 140 Google Scholar
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