Gamma radiation driven by ultra-intense and ultra-short lasers
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摘要: 伽马射线作为能量极高、穿透力极强的电磁波,在核物理、天体物理、高能物理、医疗健康及材料科学等众多前沿领域具有不可替代的重要价值。超强超短激光技术的发展,使得激光驱动的新型伽马射线源实现突破性进展。基于激光与等离子体相互作用方案能够产生高亮度、准直的飞秒级超短脉冲伽马射线,且该方案在装置紧凑性方面具备显著的优势。本文系统分析了激光驱动的数百keV至数十MeV伽马辐射的物理机制,重点讨论了逆康普顿散射、轫致辐射、Betatron辐射三类主要产生机制的特性,梳理了我国在该领域的主要研究进展及诊断技术。研究表明,通过优化激光与物质相互作用参数,可有效调控伽马射线的亮度、脉冲宽度及能谱特性。
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关键词:
- 超强超短激光 /
- 逆康普顿散射 /
- 轫致辐射 /
- Betatron辐射 /
- 能谱诊断
Abstract: Gamma rays, as electromagnetic waves with extremely high energy and exceptional penetrating power, play an irreplaceable role in numerous frontier fields including nuclear physics, astrophysics, high-energy physics, healthcare, and materials science. Advancements in ultra-intense, ultra-short laser technology have enabled breakthrough progress in laser-driven novel gamma-ray sources. Schemes based on laser-plasma interactions can generate high-brightness, collimated femtosecond-scale ultra-short pulse gamma rays, while also exhibiting significant advantages in compact device design. This paper systematically analyzes the physical mechanisms of laser-driven gamma radiation in the range of hundreds of keV to tens of MeV. It focuses on the characteristics of three primary generation mechanisms: inverse Compton scattering, bremsstrahlung, and betatron radiation. The paper reviews major research advances in China within this field and diagnostic techniques. Research indicates that by optimizing laser-matter interaction parameters, the brightness, pulse width, and energy spectrum characteristics of gamma rays can be effectively controlled. -
图 5 双光束平台的实验布局不同加速长度或等离子体密度下电子束的诊断结果及国际上相关的实验进展主导机制
Figure 5. Experimental setup of the dual-beam platform, diagnosis results of the electron beam with different acceleration lengths or plasma densities (from b1 to b5, the corresponding plasma densities are 2.4×$ {10}^{18} $, 2×$ {10}^{18} $, 2×$ {10}^{18} $, 2×$ {10}^{18} $ and 3.6×$ {10}^{18} $ $ {\text{cm}}^{-3} $, respectively, with acceleration lengths of 10, 9.5, 9, 8 and 8 mm) and the relevant international experimental progress (the solid-colored sections represent experiments that have been completed or are currently planned, while the hollow elliptical regions correspond to the parameter ranges associated with the three phases discussed in Ref.[45], the ranges corresponding to the classical radiation-dominated regime (CRDR) and the quantum radiation-dominated regime (QRDR) are indicated)
表 1 代表性激光驱动辐射源实验所用激光参数、转换靶参数及获得的$ \mathrm{X}/\gamma $射线参数
Table 1. Laser parameters,converter target parameters,and obtained $ \mathrm{X}/\gamma $-ray parameters for representative laser-driven radiation source experiments
schemes laser energy/J pulse width/fs target divergence yield/(ph/shot) photon energy/MeV year (Ref.) ICS 6.6 33 20 $ \text{μm} $ Ti/30 $ \text{μm} $ Al 4 mrad (4.8±0.3)×$ {10}^{7} $ 0.3~2.0, peak 2016
[23]1.7
0.1~2.135
372, 4 mm, He gas jet 14 mrad× 7 mrad >2×$ {10}^{8} $(max) N/A
>500 th harmonics2017
[21]3.3 33 20 $ \text{μm} $ Ti/30 $ \text{μm} $ Al 3.8 mrad×4.3 mrad 2×$ {10}^{7} $ 1.07±0.12/
0.59±0.082019
[25]0.4 25 1.2 mm, $ {\mathrm{N}}_{2} $ gas jet 20 mrad 4.5×$ {10}^{7} $ >0.2 2019
[26]0.45 40 2 mm, gas jet He+
0.5% N233 mrad× 4 mrad 3×$ {10}^{7} $ 0.07
average2020
[29]5
0.225 $ {\mathrm{N}}_{2} $ gas jet 3 mrad N/A >1 2025
[45]2.6
Gaussian:0.26
LG:0.11525 1 × 4 mm,
gas jet He+0.2%$ {\mathrm{N}}_{2} $LP-Gaussian:
(3.5 ± 0.2) mrad
CP-Gaussian:
(3.0 ± 0.2) mrad
LP-LG:
(4.2 ± 0.6) mrad
CP-LG:
(5.3 ± 0.7) mradN/A Gaussian:0.5
LG:
0.82026
[48]bremsstrahlung 14 45 2~6 mm Cu N/A >$ 10{^{10}} $ 15, peak 2017
[62]600
1501 ns
1 ps2 mm Au N/A $ {10}^{6} $~$ {10}^{7} $ 0.2-2 2022
[66]4 30 2 mm Ta N/A (1.6~1.84)×$ {10}^{8} $ >8 2023
[65]120 1 ps 2 mm Pb 1.1°(19 mrad) 2.2×$ {10}^{11} $ >16 2023
[67]0.8 24 1-3 mm W N/A N/A MeV-scale 2024
[60]150 800 3 mm Ta (11 ± 3)°
(192 mrad)7.7×$ {10}^{10} $ MeV−1·Sr−1 17 ± 2 2026
[64]Betatron 3 40 He/$ {\mathrm{N}}_{2} $ gas jet 6 mrad×3 mrad 8×$ {10}^{8} $ 75, peak 2016
[83]3.3 33 0.8 mm+3 mm,
He gas jet2.8 mrad× 2.2 mrad
with TSF, it gets larger2.1×$ {10}^{8} $ 26, peak 2018
[78]26 ± 2 21 ± 1 CNT 50° $ {10}^{12} $ 10 keV~1 MeV 2023
[86] -
[1] Tajima T, Dawson J M. Laser electron accelerator[J]. Physical Review Letters, 1979, 43(4): 267-270. doi: 10.1103/PhysRevLett.43.267 [2] Strickland D, Mourou G. Compression of amplified chirped optical pulses[J]. Optics Communications, 1985, 55(6): 447-449. doi: 10.1016/0030-4018(85)90151-8 [3] Mangles S P D, Murphy C D, Najmudin Z, et al. Monoenergetic beams of relativistic electrons from intense laser–plasma interactions[J]. Nature, 2004, 431(7008): 535-538. doi: 10.1038/nature02939 [4] Leemans W P, Nagler B, Gonsalves A J, et al. GeV electron beams from a centimetre-scale accelerator[J]. Nature Physics, 2006, 2(10): 696-699. doi: 10.1038/nphys418 [5] Mourou G, Tajima T. More intense, shorter pulses[J]. Science, 2011, 331(6013): 41-42. doi: 10.1126/science.1200292 [6] Krausz F, Brabec T, Schnürer M, et al. Extreme nonlinear optics: exposing matter to a few periods of light[J]. Optics and Photonics News, 1998, 9(7): 46-51. doi: 10.1364/opn.9.7.000046 [7] Esarey E, Schroeder C B, Leemans W P. Physics of laser-driven plasma-based electron accelerators[J]. Reviews of Modern Physics, 2009, 81(3): 1229-1285. doi: 10.1103/RevModPhys.81.1229 [8] Malka V, Faure J, Gauduel Y A, et al. Principles and applications of compact laser–plasma accelerators[J]. Nature Physics, 2008, 4(6): 447-453. doi: 10.1038/nphys966 [9] Zhu Qihua, Zhou Kainan, Su Jingqin, et al. The Xingguang-III laser facility: precise synchronization with femtosecond, picosecond and nanosecond beams[J]. Laser Physics Letters, 2018, 15: 015301. doi: 10.1088/1612-202X/aa94e9 [10] Gan Zebiao, Yu Lianghong, Wang Cheng, et al. The Shanghai superintense ultrafast laser facility (SULF) project[M]//Yamanouchi K, Midorikawa K, Roso L. Progress in Ultrafast Intense Laser Science XVI. Cham: Springer, 2021: 199-217. [11] 曾沛颖, 汤晓云, 杨学东, 等. 神光Ⅱ激光装置集中控制系统设计[J]. 强激光与粒子束, 2012, 24(11): 2595-2598 doi: 10.3788/HPLPB20122411.2595Zeng Peiying, Tang Xiaoyun, Yang Xuedong, et al. Design of Shenguang-Ⅱ facility centralized control system[J]. High Power Laser and Particle Beams, 2012, 24(11): 2595-2598 doi: 10.3788/HPLPB20122411.2595 [12] Wu Yuchi, Zhu Bin, Dong Kegong, et al. XingGuang III laser facility and its experimental ability to drive high-energy particle beams[J]. Laser Physics, 2020, 30: 096001. doi: 10.1088/1555-6611/aba3ca [13] 李毅飞, 陈黎明. 飞秒激光驱动的超快X射线辐射(特邀)[J]. 中国激光, 2025, 52: 2301016 doi: 10.3788/CJL251399Li Yifei, Chen Liming. Femtosecond laser-driven ultrafast X-ray radiation (invited)[J]. Chinese Journal of Lasers, 2025, 52: 2301016 doi: 10.3788/CJL251399 [14] 李毅飞, 王进光, 鲁欣, 等. 飞秒激光驱动的超快X射线动力学实验站[J]. 强激光与粒子束, 2026, 38: 031004 (Li Yifei, Wang Jinguang, Lu Xin, et al. Femtosecond laser-driven ultrafast X-ray dynamics experimental station[J]. High Power Laser and Particle Beams, 2026, 38: 031004 doi: 10.11884/HPLPB202638.250382Li Yifei, Wang Jinguang, Lu Xin, et al. Femtosecond laser-driven ultrafast X-ray dynamics experimental station[J]. High Power Laser and Particle Beams, 2026, 38: 031004 doi: 10.11884/HPLPB202638.250382 [15] Li Yutong, Chen Liming, Chen Min, et al. High-intensity lasers and research activities in China[J]. High Power Laser Science and Engineering, 2025, 13: e12. doi: 10.1017/hpl.2024.69 [16] 闫文超, 朱常青, 王进光, 等. 全光汤姆孙散射[J]. 物理学报, 2021, 70: 084104 doi: 10.7498/aps.70.20210549Yan Wenchao, Zhu Changqing, Wang Jinguang, et al. All-optical Thomson scattering[J]. Acta Physica Sinica, 2021, 70: 084104 doi: 10.7498/aps.70.20210549 [17] Seipt D. Volkov states and non-linear Compton scattering in short and intense laser pulses[DB/OL]. arXiv preprint arXiv: 1701.03692, 2017. [18] Debus A, Bock S, Bussmann M, et al. Linear and non-linear Thomson-scattering x-ray sources driven by conventionally and laser plasma accelerated electrons[C]//Proceedings of SPIE 7359, Harnessing Relativistic Plasma Waves as Novel Radiation Sources from Terahertz to X-Rays and Beyond. 2009: 735908. [19] Albert F, Thomas A G R. Applications of laser Wakefield accelerator-based light sources[J]. Plasma Physics and Controlled Fusion, 2016, 58: 103001. doi: 10.1088/0741-3335/58/10/103001 [20] Ritus V I. Quantum effects of the interaction of elementary particles with an intense electromagnetic field[J]. Journal of Soviet Laser Research, 1985, 6(5): 497-617. doi: 10.1007/BF01120220 [21] Yan Wenchao, Fruhling C, Golovin G, et al. High-order multiphoton Thomson scattering[J]. Nature Photonics, 2017, 11(8): 514-520. doi: 10.1038/nphoton.2017.100 [22] Ta Phuoc K, Corde S, Thaury C, et al. All-optical Compton gamma-ray source[J]. Nature Photonics, 2012, 6(5): 308-311. doi: 10.1038/nphoton.2012.82 [23] Yu Changhai, Qi Rong, Wang Wentao, et al. Ultrahigh brilliance quasi-monochromatic MeV γ-rays based on self-synchronized all-optical Compton scattering[J]. Scientific Reports, 2016, 6: 29518. doi: 10.1038/srep29518 [24] 余昌海, 秦志勇, 张志钧, 等. 激光尾波场电子加速及新型辐射源(特邀)[J]. 中国激光, 2024, 51: 0101002 doi: 10.3788/CJL231403Yu Changhai, Qin Zhiyong, Zhang Zhijun, et al. Laser wakefield electron acceleration and novel radiation sources (invited)[J]. Chinese Journal of Lasers, 2024, 51: 0101002 doi: 10.3788/CJL231403 [25] Wu Ying, Yu Changhai, Qin Zhiyong, et al. Dual-color γ-rays via all-optical Compton scattering from a cascaded laser-driven wakefield accelerator[J]. Plasma Physics and Controlled Fusion, 2019, 61: 085030. doi: 10.1088/1361-6587/ab29d9 [26] Zhu Changqing, Wang Jinguang, Feng Jie, et al. Inverse Compton scattering X-ray source from laser electron accelerator in pure nitrogen with 15 TW laser pulses[J]. Plasma Physics and Controlled Fusion, 2019, 61: 024001. doi: 10.1088/1361-6587/aaebe3 [27] Feng Jie, Wang Jinguang, Li Yifei, et al. Intense γ ray generated by refocusing laser pulse on Wakefield accelerated electrons[J]. Physics of Plasmas, 2017, 24: 093110. doi: 10.1063/1.4994710 [28] Chen Liming, Hu Xichen, Zhu Mingyang, et al. Enhanced inverse Compton scattering via spontaneous focusing induced by coated plasma mirror[EB/OL]. 2025(2025-12-11). https://www.researchsquare.com/article/rs-8076863/v1?utm_source=researchgate.net&utm_medium=article. [29] Ma Yue, Hua Jianfei, Liu Dexiang, et al. Region-of-interest micro-focus computed tomography based on an all-optical inverse Compton scattering source[J]. Matter and Radiation at Extremes, 2020, 5: 064401. doi: 10.1063/5.0016034 [30] Ma Yue, Liu Dexiang, Hua Jianfei, et al. Dual-energy micro-focus computed tomography based on the energy-angle correlation of inverse Compton scattering source[J]. Journal of X-Ray Science and Technology, 2023, 31(6): 1227-1243. doi: 10.3233/xst-230093 [31] Guo Bo, Wu Shuanghua, Ma Yue, et al. X-ray phase-contrast imaging using a quasi-monochromatic all-optical inverse Compton scattering source[J]. Matter and Radiation at Extremes, 2026, 11: 017601. doi: 10.1063/5.0281386 [32] Wang Weimin, Sheng Zhengming, Gibbon P, et al. Collimated ultrabright gamma rays from electron wiggling along a petawatt laser-irradiated wire in the QED regime[J]. Proceedings of the National Academy of Sciences of the United States of America, 2018, 115(40): 9911-9916. [33] Gonoskov A, Blackburn T G, Marklund M, et al. Charged particle motion and radiation in strong electromagnetic fields[J]. Reviews of Modern Physics, 2022, 94: 045001. doi: 10.1103/RevModPhys.94.045001 [34] Matheron A, Marquès J R, Lelasseux V, et al. Compton photons at the GeV scale from self-aligned collisions with a plasma mirror[DB/OL]. arXiv preprint arXiv: 2412.19337, 2024. [35] Danson C N, Haefner C, Bromage J, et al. Petawatt and exawatt class lasers worldwide[J]. High Power Laser Science and Engineering, 2019, 7: e54. doi: 10.1017/hpl.2019.36 [36] Sarri G, Corvan D J, Schumaker W, et al. Ultrahigh brilliance multi-MeV γ-ray beams from nonlinear relativistic Thomson scattering[J]. Physical Review Letters, 2014, 113: 224801. doi: 10.1103/PhysRevLett.113.224801 [37] Chen S, Powers N D, Ghebregziabher I, et al. MeV-energy X rays from inverse Compton scattering with laser-Wakefield accelerated electrons[J]. Physical Review Letters, 2013, 110: 155003. doi: 10.1103/PhysRevLett.110.155003 [38] Powers N D, Ghebregziabher I, Golovin G, et al. Quasi-monoenergetic and tunable X-rays from a laser-driven Compton light source[J]. Nature Photonics, 2014, 8(1): 28-31. doi: 10.1038/nphoton.2013.314 [39] Liu Cheng, Golovin G, Chen Shouyuan, et al. Generation of 9 MeV γ-rays by all-laser-driven Compton scattering with second-harmonic laser light[J]. Optics Letters, 2014, 39(14): 4132-4135. doi: 10.1364/OL.39.004132 [40] Khrennikov K, Wenz J, Buck A, et al. Tunable all-optical quasimonochromatic Thomson X-ray source in the nonlinear regime[J]. Physical Review Letters, 2015, 114: 195003. doi: 10.1103/PhysRevLett.114.195003 [41] Cole J M, Symes D R, Lopes N C, et al. High-resolution μCT of a mouse embryo using a compact laser-driven X-ray betatron source[J]. Proceedings of the National Academy of Sciences of the United States of America, 2018, 115(25): 6335-6340. [42] Cole J M, Behm K T, Blackburn T G, et al. Experimental observation of radiation reaction in the collision of a high-intensity laser pulse with a laser-Wakefield accelerated electron beam[DB/OL]. arXiv preprint arXiv: 1707.06821, 2017. [43] Poder K, Tamburini M, Sarri G, et al. Experimental signatures of the quantum nature of radiation reaction in the field of an ultraintense laser[J]. Physical Review X, 2018, 8: 031004. [44] Mirzaie M, Hojbota C I, Kim D Y, et al. All-optical nonlinear Compton scattering performed with a multi-petawatt laser[J]. Nature Photonics, 2024, 18(11): 1212-1217. doi: 10.1038/s41566-024-01550-8 [45] Chen Siyu, Yan Wenchao, Zhu Mingyang, et al. A platform for all-optical Thomson/Compton scattering with versatile parameters[J]. High Power Laser Science and Engineering, 2025, 13: e56. doi: 10.1017/hpl.2025.36 [46] Zhou Weijun, Yan Wenchao, Wang Jinguang, et al. Gamma-ray vortex burst in nonlinear Thomson scattering with refocusing spiral plasma mirror[J]. Ultrafast Science, 2023, 3: 0005. doi: 10.34133/ultrafastscience.0005 [47] Jiang Jingjing, Zhuang Kaihong, Chen Jiading, et al. Controlling the polarization and vortex charge of γ photons via nonlinear Compton scattering[J]. Physical Review Letters, 2025, 134: 153802. doi: 10.1103/PhysRevLett.134.153802 [48] Wei Mingxuan, Chen Siyu, Wang Yu, et al. Experimental evidence of vortex $ \gamma $ photons in all-optical inverse Compton scattering[J]. Physical Review Letters, 2026, 136: 025001. doi: 10.1103/92v4-bzp2 [49] 沈百飞. 强场激光物理[M]. 北京: 科学出版社, 2023Shen Baifei. High-field laser physics. [M]: Beijing: Science Press [50] Palaniyappan S, Gautier D C, Tobias B J, et al. MeV bremsstrahlung X rays from intense laser interaction with solid foils[J]. Laser and Particle Beams, 2018, 36(4): 502-506. doi: 10.1017/S0263034618000551 [51] Compant La Fontaine A, Courtois C, Lefebvre E. Production of multi-MeV Bremsstrahlung X-ray sources by petawatt laser pulses on various targets[J]. Physics of Plasmas, 2012, 19: 023104. doi: 10.1063/1.3680611 [52] Tavana P, Bukharskii N, Gyrdymov M, et al. Ultra-high efficiency bremsstrahlung production in the interaction of direct laser-accelerated electrons with high-Z material[J]. Frontiers in Physics, 2023, 11: 1178967. doi: 10.3389/fphy.2023.1178967 [53] Noh Y, Song J, Mirzaie M, et al. Charge-neutral, GeV-scale electron-positron pair beams produced using bremsstrahlung gamma rays[J]. Communications Physics, 2024, 7: 44. doi: 10.1038/s42005-024-01527-7 [54] Lemos N, Albert F, Shaw J L, et al. Bremsstrahlung hard x-ray source driven by an electron beam from a self-modulated laser Wakefield accelerator[J]. Plasma Physics and Controlled Fusion, 2018, 60: 054008. doi: 10.1088/1361-6587/aab3b5 [55] Courtois C, Edwards R, Compant La Fontaine A, et al. High-resolution multi-MeV x-ray radiography using relativistic laser-solid interaction[J]. Physics of Plasmas, 2011, 18: 023101. doi: 10.1063/1.3551738 [56] Perry M D, Sefcik J A, Cowan T, et al. Hard x-ray production from high intensity laser solid interactions (invited)[J]. Review of Scientific Instruments, 1999, 70(1): 265-269. doi: 10.1063/1.1149442 [57] Cipiccia S, Wiggins S M, Shanks R P, et al. A tuneable ultra-compact high-power, ultra-short pulsed, bright gamma-ray source based on bremsstrahlung radiation from laser-plasma accelerated electrons[J]. Journal of Applied Physics, 2012, 111: 063302. doi: 10.1063/1.3693537 [58] Armstrong C D, Brenner C M, Jones C, et al. Bremsstrahlung emission from high power laser interactions with constrained targets for industrial radiography[J]. High Power Laser Science and Engineering, 2019, 7: e24. doi: 10.1017/hpl.2019.8 [59] Prencipe I, Metzkes-Ng J, Pazzaglia A, et al. Efficient laser-driven proton and bremsstrahlung generation from cluster-assembled foam targets[J]. New Journal of Physics, 2021, 23: 093015. doi: 10.1088/1367-2630/ac1fcd [60] Wu Yuchi, Wang Shaoyi, Zhu Bin, et al. Virtual source approach for maximizing resolution in high-penetration gamma-ray imaging[J]. Matter and Radiation at Extremes, 2024, 9: 037202. doi: 10.1063/5.0179781 [61] Döpp A, Guillaume E, Thaury C, et al. A bremsstrahlung gamma-ray source based on stable ionization injection of electrons into a laser Wakefield accelerator[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2016, 830: 515-519. [62] Li Shun, Shen Baifei, Xu Jiancai, et al. Ultrafast multi-MeV gamma-ray beam produced by laser-accelerated electrons[J]. Physics of Plasmas, 2017, 24: 093104. doi: 10.1063/1.4996020 [63] Cao Zongwei, Qi Wei, Lan Haoyang, et al. Experimental study of medical isotopes 62, 64Cu and 68Ga production using intense picosecond laser pulse[J]. Plasma Physics and Controlled Fusion, 2023, 65: 055007. doi: 10.1088/1361-6587/acc090 [64] Yang Mingzhe, Wang Ziyao, Ren Jieru, et al. Express diagnostic of intense laser-driven MeV radiation source using copper isotopes[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2026, 1084: 171188. doi: 10.1016/j.nima.2025.171188 [65] Wu D, Lan H Y, Zhang J Y, et al. New measurements of 92Mo (γ, n) and (γ, 3n) reactions using laser-driven bremsstrahlung γ-ray[J]. Frontiers in Physics, 2023, 11: 1178257. doi: 10.3389/fphy.2023.1178257 [66] 熊俊, 安红海, 王琛, 等. 长短脉冲联合驱动双层结构靶优化伽马射线的产生[J]. 物理学报, 2022, 71: 215201 doi: 10.7498/aps.71.20212042Xiong Jun, An Honghai, Wang Chen, et al. Gamma-ray generation optimized by long and short pulses jointly driving double-layer target[J]. Acta Physica Sinica, 2022, 71: 215201 doi: 10.7498/aps.71.20212042 [67] Fan Lulin, Xu Tongjun, Li Shun, et al. Collimated gamma beams with high peak flux driven by laser-accelerated electrons[J]. High Power Laser Science and Engineering, 2023, 11: e26. doi: 10.1017/hpl.2023.25 [68] Hollinger R, Wang Shoujun, Zahedpour Anaraki S, et al. Laser-driven high-resolution MeV x-ray tomography[J]. Optica, 2025, 12(3): 433-436. doi: 10.1364/OPTICA.542536 [69] Albert F, Thomas A G R, Mangles S P D, et al. Laser Wakefield accelerator based light sources: potential applications and requirements[J]. Plasma Physics and Controlled Fusion, 2014, 56: 084015. doi: 10.1088/0741-3335/56/8/084015 [70] Wang Shuoqin, Clayton C E, Blue B E, et al. X-ray emission from betatron motion in a plasma wiggler[J]. Physical Review Letters, 2002, 88: 135004. doi: 10.1103/PhysRevLett.88.135004 [71] Rousse A, Phuoc K T, Shah R, et al. Production of a keV X-ray beam from synchrotron radiation in relativistic laser-plasma interaction[J]. Physical Review Letters, 2004, 93: 135005. doi: 10.1103/PhysRevLett.93.135005 [72] Phuoc K T, Burgy F, Rousseau J P, et al. Laser based synchrotron radiation[J]. Physics of Plasmas, 2005, 12: 023101. doi: 10.1063/1.1842755 [73] Phuoc K T, Corde S, Shah R, et al. Imaging electron trajectories in a laser-Wakefield cavity using betatron x-ray radiation[J]. Physical Review Letters, 2006, 97: 225002. doi: 10.1103/PhysRevLett.97.225002 [74] Albert F, Shah R, Phuoc K T, et al. Betatron oscillations of electrons accelerated in laser Wakefields characterized by spectral x-ray analysis[J]. Physical Review E, 2008, 77: 056402. doi: 10.1103/PhysRevE.77.056402 [75] Lu W, Tzoufras M, Joshi C, et al. Generating multi-GeV electron bunches using single stage laser Wakefield acceleration in a 3D nonlinear regime[J]. Physical Review Special Topics—Accelerators and Beams, 2007, 10: 061301. doi: 10.1103/PhysRevSTAB.10.061301 [76] Cipiccia S, Islam M R, Ersfeld B, et al. Gamma-rays from harmonically resonant betatron oscillations in a plasma wake[J]. Nature Physics, 2011, 7(11): 867-871. doi: 10.1038/nphys2090 [77] Ferri J, Corde S, Döpp A, et al. High-brilliance betatron γ-ray source powered by laser-accelerated electrons[J]. Physical Review Letters, 2018, 120: 254802. doi: 10.1103/PhysRevLett.120.254802 [78] Yu Changhai, Liu Jiansheng, Wang Wentao, et al. Enhanced Betatron radiation by steering a laser-driven plasma Wakefield with a tilted shock front[J]. Applied Physics Letters, 2018, 112: 133503. doi: 10.1063/1.5019406 [79] Kozlova M, Andriyash I, Gautier J, et al. Hard X rays from laser-Wakefield accelerators in density tailored plasmas[J]. Physical Review X, 2020, 10: 011061. doi: 10.1103/physrevx.10.011061 [80] Dong C F, Zhao T Z, Behm K, et al. High flux femtosecond x-ray emission from the electron-hose instability in laser Wakefield accelerators[J]. Physical Review Accelerators and Beams, 2018, 21: 041303. doi: 10.1103/PhysRevAccelBeams.21.041303 [81] Chen L M, Yan W C, Li D Z, et al. Bright betatron X-ray radiation from a laser-driven-clustering gas target[J]. Scientific Reports, 2013, 3: 1912. doi: 10.1038/srep01912 [82] Li Y F, Feng J, Tan J H, et al. Electron beam and betatron x-ray generation in a hybrid electron accelerator driven by high intensity picosecond laser pulses[J]. High Energy Density Physics, 2020, 37: 100859. doi: 10.1016/j.hedp.2020.100859 [83] Huang K, Li Y F, Li D Z, et al. Resonantly enhanced betatron hard x-rays from ionization injected electrons in a laser plasma accelerator[J]. Scientific Reports, 2016, 6: 27633. doi: 10.1038/srep27633 [84] Rocca J J, Capeluto M G, Hollinger R C, et al. Ultra-intense femtosecond laser interactions with aligned nanostructures[J]. Optica, 2024, 11(3): 437-453. doi: 10.1364/OPTICA.510542 [85] Shou Yinren, Wang Pengjie, Lee S G, et al. Brilliant femtosecond-laser-driven hard X-ray flashes from carbon nanotube plasma[J]. Nature Photonics, 2023, 17(2): 137-142. doi: 10.1038/s41566-022-01114-8 [86] Zhang Liangqi, Wu Shaodong, Huang Hairong, et al. Brilliant attosecond γ-ray emission and high-yield positron production from intense laser-irradiated Nano-micro array[J]. Physics of Plasmas, 2021, 28: 023110. doi: 10.1063/5.0030909 [87] Babjak R, Vranic M. Betatron radiation emitted during the direct laser acceleration of electrons in underdense plasmas[J]. Plasma Physics and Controlled Fusion, 2025, 67: 085019. doi: 10.1088/1361-6587/adf50b [88] Zhu Xinglong, Chen Min, Weng Suming, et al. Extremely brilliant GeV γ-rays from a two-stage laser-plasma accelerator[J]. Science Advances, 2020, 6: eaaz7240. doi: 10.1126/sciadv.aaz7240 [89] Kim H T, Mirzaie M, Pae K H, et al. Enhanced gamma-ray betatron radiation from laser accelerator and plasma radiator[EB/OL]. 2025(2025-10-15). https://assets-eu.researchsquare.com/files/rs-7559872/v1_covered_723ead29-5214-4f10-bf3d-e6c14b4c4862.pdf?c=1767197558. [90] Behrens R. A spectrometer for pulsed and continuous photon radiation[J]. Journal of Instrumentation, 2009, 4: P03027. doi: 10.1088/1748-0221/4/03/p03027 [91] Scott R H H, Clark E L, Pérez F, et al. Measuring fast electron spectra and laser absorption in relativistic laser-solid interactions using differential bremsstrahlung photon detectors[J]. Review of Scientific Instruments, 2013, 84: 083505. doi: 10.1063/1.4816332 [92] Jeon J H, Nakajima K, Kim H T, et al. A broadband gamma-ray spectrometry using novel unfolding algorithms for characterization of laser Wakefield-generated betatron radiation[J]. Review of Scientific Instruments, 2015, 86: 123116. doi: 10.1063/1.4939014 [93] Westover B, Chen C D, Patel P K, et al. Characterization of the fast electrons distribution produced in a high intensity laser target interaction[J]. Physics of Plasmas, 2014, 21: 031212. doi: 10.1063/1.4865371 [94] Albert F, Pollock B B, Shaw J L, et al. Measuring the angular dependence of betatron x-ray spectra in a laser-Wakefield accelerator[J]. Plasma Physics and Controlled Fusion, 2014, 56: 084016. doi: 10.1088/0741-3335/56/8/084016 [95] Hannasch A, Laso Garcia A, LaBerge M, et al. Compact spectroscopy of keV to MeV X-rays from a laser Wakefield accelerator[J]. Scientific Reports, 2021, 11: 14368. doi: 10.1038/s41598-021-93689-5 [96] Fauvel G, Tangtartharakul K, Arefiev A, et al. Compact in-vacuum gamma-ray spectrometer for high-repetition rate PW-class laser–matter interaction[J]. Review of Scientific Instruments, 2025, 96: 023102. doi: 10.1063/5.0206348 [97] 于明海, 谭放, 闫永宏, 等. 用于激光产生的高能X射线源能谱诊断的滤片堆栈谱仪的研制[J]. 原子能科学技术, 2017, 51(6): 1090-1095 doi: 10.7538/yzk.2017.51.06.1090Yu Minghai, Tan Fang, Yan Yonghong, et al. Development of filter stack spectrometer for spectrum measurement of x ray generated by laser[J]. Atomic Energy Science and Technology, 2017, 51(6): 1090-1095 doi: 10.7538/yzk.2017.51.06.1090 [98] Wong C S, Strehlow J, Broughton D P, et al. Robust unfolding of MeV x-ray spectra from filter stack spectrometer data[J]. Review of Scientific Instruments, 2024, 95: 023301. doi: 10.1063/5.0190679 [99] Rusby D R, Williams G J, Kerr S M, et al. Diagnostic development and needs for laser driven MeV x-ray radiography[J]. Review of Scientific Instruments, 2024, 95: 123512. doi: 10.1063/5.0219493 [100] Behm K T, Cole J M, Joglekar A S, et al. A spectrometer for ultrashort gamma-ray pulses with photon energies greater than 10 MeV[J]. Review of Scientific Instruments, 2018, 89: 113303. doi: 10.1063/1.5056248 [101] Liang E, Zheng K Q, Yao K, et al. A scintillator attenuation spectrometer for intense gamma-rays[J]. Review of Scientific Instruments, 2022, 93: 063103. doi: 10.1063/5.0082131 [102] Corvan D J, Sarri G, Zepf M. Design of a compact spectrometer for high-flux MeV gamma-ray beams[J]. Review of Scientific Instruments, 2014, 85: 065119. doi: 10.1063/1.4884643 [103] Zhang Zhenchi, Yang Tao, Hu Guangyue, et al. Compact broadband high-resolution Compton spectroscopy for laser-driven high-flux gamma rays[J]. Matter and Radiation at Extremes, 2021, 6: 014401. doi: 10.1063/5.0026005 [104] Yadav M, Oruganti M H, Naranjo B, et al. Reconstruction of beam parameters and betatron radiation spectra measured with a Compton spectrometer[J]. Physical Review Accelerators and Beams, 2025, 28: 042802. doi: 10.1103/PhysRevAccelBeams.28.042802 [105] Singh S, Versaci R, Laso Garcia A, et al. Compact high energy x-ray spectrometer based on forward Compton scattering for high intensity laser plasma experiments[J]. Review of Scientific Instruments, 2018, 89: 085118. doi: 10.1063/1.5040979 [106] Haden D, Golovin G, Yan W, et al. High energy X-ray Compton spectroscopy via iterative reconstruction[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2020, 951: 163032. doi: 10.1016/j.nima.2019.163032 [107] Yang Tao, Hu Guangyue, Li Mengting, et al. Compact broadband Compton spectroscopy used for intense laser-driven gamma rays[J]. Review of Scientific Instruments, 2021, 92: 053546. doi: 10.1063/5.0028098 [108] Fleck K, Cavanagh N, Sarri G. Conceptual design of a high-flux multi-GeV gamma-ray spectrometer[J]. Scientific Reports, 2020, 10: 9894. doi: 10.1038/s41598-020-66832-x [109] Cavanagh N, Fleck K, Streeter M J V, et al. Experimental characterization of a single-shot spectrometer for high-flux, GeV-scale gamma-ray beams[J]. Physical Review Research, 2023, 5: 043046. doi: 10.1103/PhysRevResearch.5.043046 [110] LUXE Collaboration, Abramowicz H, Almanza Soto M, et al. Technical design report for the LUXE experiment[J]. The European Physical Journal Special Topics, 2024, 233(10): 1709-1974. doi: 10.1140/epjs/s11734-024-01164-9 [111] Zhang Zhuofan, Wei Mingxuan, Fleck K, et al. Neural network-based deconvolution for GeV-scale gamma-ray spectroscopy[DB/OL]. arXiv preprint arXiv: 2512.01612, 2025. [112] Ma Yue, Hua Jianfei, Liu Dexiang, et al. Compact polarized X-ray source based on all-optical inverse Compton scattering[J]. Physical Review Applied, 2023, 19: 014073. doi: 10.1103/PhysRevApplied.19.014073 [113] Taira Y, Yang Yuxuan, Shizuma T, et al. Generation and measurement of gamma rays with axially symmetric polarization states via Compton scattering[J]. Physical Review Research, 2025, 7: 033130. doi: 10.1103/pn68-rjd2 [114] Taira Y, Endo S, Kawamura S, et al. Measurement of the spatial polarization distribution of circularly polarized gamma rays produced by inverse Compton scattering[J]. Physical Review A, 2023, 107: 063503. doi: 10.1103/PhysRevA.107.063503 [115] Go S, Tsuzuki Y, Yoneda H, et al. Demonstration of nuclear gamma-ray polarimetry based on a multi-layer CdTe Compton camera[J]. Scientific Reports, 2024, 14: 2573. doi: 10.1038/s41598-024-52692-2 [116] Depaola G O, Kozameh C N. Detecting polarized gamma-rays by pair production[J]. Radiation Physics and Chemistry, 1998, 53(5): 455-459. doi: 10.1016/S0969-806X(98)00212-6 [117] Depaola G O, Kozameh C N, Tiglio M H. A method to determine the polarization of high energy gamma rays[J]. Astroparticle Physics, 1999, 10(2/3): 175-183. doi: 10.1016/s0927-6505(98)00054-1 [118] Bloser P F, Hunter S D, Depaola G O, et al. A concept for a high-energy gamma-ray polarimeter[C]//Proceedings of SPIE 5165, X-Ray and Gamma-Ray Instrumentation for Astronomy XIII. 2003: 322-333. -
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