All-optical Thomson scattering

Yan Wen-Chao; Zhu Chang-Qing; Wang Jin-Guang; Feng Jie; Li Yi-Fei; Tan Jun-Hao; Chen Li-Ming

doi:10.7498/aps.70.20210319

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:

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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References

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Cited By

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

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

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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

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

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图 3 等离子体镜方案产生X射线的示意图

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

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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

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

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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

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

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图 6 文献[35]报道的高阶多光子效应

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

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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

Figure 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]

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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

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[1]	Thomson J 1899 The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science 47 253 Google Scholar
[2]	Barkla C G 1903 Proc. Phys. Soc. London 19 185 Google Scholar
[3]	Barkla C G 1903 The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science 5 685 Google Scholar
[4]	Stephenson R J 1967 Am. J. Phys. 35 140 Google Scholar
[5]	Compton A H 1923 Phys. Rev. 21 483 Google Scholar
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[8]	Woo Y H 1930 Proc. Natl. Acad. Sci. U.S.A. 16 814 Google Scholar
[9]	Woo Y H 1931 Proc. Natl. Acad. Sci. U.S.A. 17 470 Google Scholar
[10]	Woo Y H 1931 Proc. Natl. Acad. Sci. U.S.A. 17 467 Google Scholar
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[23]	Geddes C G R, Toth C, van Tilborg J, Esarey E, Schroeder C B, Bruhwiler D, Nieter C, Cary J, Leemans W P 2004 Nature 431 538 Google Scholar
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[28]	Papadopoulos D N, Zou J P, Blanc C L, Chériaux G, Georges P, Druon F, Mennerat G, Ramirez P, Martin L, Fréneaux A, Beluze A, Lebas N, Monot P, Mathieu F, Audebert P 2016 High Power Laser Sci. Eng. 4 e34 Google Scholar
[29]	Shen B, Bu Z, Xu J, Xu T, Ji L, Li R, Xu Z 2018 Plasma Phys. Controlled Fusion 60 044002 Google Scholar
[30]	Danson C N, Haefner C, Bromage J, Butcher T, Chanteloup J C F, Chowdhury E A, Galvanauskas A, Gizzi L A, Hein J, Hillier D I, Hopps N W, Kato Y, Khazanov E A, Kodama R, Korn G, Li R X, Li Y T, Limpert J, Ma J G, Nam C H, Neely D, Papadopoulos D, Penman R R, Qian L J, Rocca J J, Shaykin A A, Siders C W, Spindloe C, Szatmari S, Trines R, Zhu J Q, Zhu P, Zuegel J D 2019 High Power Laser Science and Engineering 7 e54 Google Scholar
[31]	Chu Y, Gan Z, Liang X, Yu L, Lu X, Wang C, Wang X, Xu L, Lu H, Yin D 2015 Opt. Lett. 40 5011 Google Scholar
[32]	Zamfir N V 2014 Eur. Phys. J.-Spec. Top. 223 1221 Google Scholar
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[34]	Weber S, Bechet S, Borneis S, Brabec L, Bučka M, Chacon-Golcher E, Ciappina M, DeMarco M, Fajstavr A, Falk K 2018 Matter Radiat. Extremes 2 149
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