Research progress of ultrabright <i>γ</i>-ray radiation and electron-positron pair production driven by extremely intense laser fields

Zhu Xing-Long; Wang Wei-Min; Yu Tong-Pu; He Feng; Chen Min; Weng Su-Ming; Chen Li-Ming; Li Yu-Tong; Sheng Zheng-Ming; Zhang Jie

doi:10.7498/aps.70.20202224

Abstract

The advent of high-power ultra-short ultra-intense laser pulses opens up the new frontiers of relativistic nonlinear optics, high-field physics, laser-driven inertial confined fusion, etc. In recent years, with the construction of high power laser facilities at a multi-petawatt (PW) level and above, the interaction between laser and matter enters into a new realm of high field physics, where extremely rich nonlinear physics is involved. In addition to classical nonlinear physics involving wave-particle interactions, relativistic effects, and ponderomotive force effects, the quantum electrodynamic (QED) effects occur, such as radiation reaction force, electron-positron pair production, strong γ-ray radiation, QED cascades, and vacuum polarization. This paper presents a brief overview of electron-positron pair creation and bright γ-ray emission driven by the extremely intense laser fields.

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.
Department of Physics, Renmin University of China, Beijing 100872, China
3.
Collaborative Innovation Center for IFSA, Shanghai Jiao Tong University, Shanghai 200240, China
4.
Department of Physics, National University of Defense Technology, Changsha 410073, China
5.
Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
6.
Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai 200240, China

Corresponding author: Wang Wei-Min, weiminwang1@ruc.edu.cn ; Sheng Zheng-Ming, zmsheng@sjtu.edu.cn ;

Funds: Project supported by the National Key R&D Program of China (Grant Nos. 2018YFA0404802, 2018YFA0404801), the National Natural Science Foundation of China (Grant Nos. 11775144, 11991074, 11975154, 11925405, 11775302, 11875319), the Strategic Priority Research Program of Chinese Academy of Sciences, China (Grant Nos. XDA25050100, XDA25050300), and the Fundamental Research Fund for the Central Universities, China (Grant No. 20XNLG01)

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References

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Cited By

图 1 聚焦激光强度随时间的发展历程及其相应的物理研究范畴^[4]

Figure 1. Progress of the focused laser intensity over years and the development of laser-driven physics^[4].

DownLoad: Full-Size Img PowerPoint

图 2 基于第三代同步辐射源、X射线自由电子激光^[47](a)和激光等离子体方法^[8] (b)所产生的X射线辐射源的峰值亮度范围

Figure 2. Peak brilliance for different types of X-ray radiation sources from the third-generation synchrotron-radiation sources and XFELs^[47] (a) and laser-plasma-based radiation sources^[8] (b).

DownLoad: Full-Size Img PowerPoint

图 3 (a)丝靶方案的示意图; (b) X射线自由电子激光装置、同步辐射装置、基于激光尾场加速器的Betatron或Compton散射光源以及该细丝靶方案产生的伽马射线源光子能量和峰值亮度的范围; (c), (d)在不同驱动激光功率条件下所产生的伽马射线源的角分布和能谱分布, 图示中“ ×10”表示光子数放大10倍^[80]

Figure 3. (a) Schematic diagram of the wire scheme; (b) chart of photon energy and brilliance of gamma-rays generated from our wire scheme, XFEL, synchrotron radiation facilities, and betatron radiation and Compton scattering based on LWFA; the angular distributions (c) and energy spectra (d) of the generated gamma-rays under different laser powers, where “ ×10” in the legend indicates the photon number multiplied by a factor of 10^[80].

DownLoad: Full-Size Img PowerPoint

图 4 (a) 利用两级激光等离子体加速器产生极高亮度伽马射线源的原理图; (b) 三维数值模拟结果; (c)伽马射线源的能谱分布和角分布; (d) 伽马射线源峰值亮度(单位: photons/(s·mm²·mrad²·0.1%BW))关于辐射光子能量的分布^[66]

Figure 4. (a) Concept of extremely brilliant γ-rays from a two-stage laser-plasma accelerator; (b) 3D simulation results of collimated γ-rays radiation in the two-stage LWFA scheme; (c) the angular-spectrum and angular distribution of the emitted gamma-rays; (d) the gamma-ray peak brilliance (photons/(s·mm²·mrad²·0.1%BW)) as a function of the radiated photon energy^[66].

DownLoad: Full-Size Img PowerPoint

图 5 (a) 圆偏振拉盖尔高斯激光驱动锥-固体薄靶产生超亮阿秒伽马射线脉冲的示意图, 在强激光场作用下, 电子(红色环)从锥壁中被周期性地拉出, 并沿着激光传播方向被加速; 随后, 聚焦的强激光场被放置在锥靶外的固体薄靶(蓝色平板)反射, 从而与加速的稠密阿秒高能电子束对撞产生数MeV光子能量的超亮阿秒伽马射线脉冲(橙绿色环); (b), (c) 入射激光场和聚焦激光场的强度分布; (d)时刻t = 14T₀处的电子密度分布; (e) 时刻t = 30T₀ 处的伽马光子密度分布^[64]

Figure 5. (a) Schematic diagram of attosecond γ-ray pulse generation from a circularly-polarized Laguerre-Gaussian laser-driven cone-foil target. Electrons (red rings) are extracted from the cone walls and accelerated by the focusing laser. Then, the focusing laser pulse is reflected by a plasma mirror/foil (blue plate) and collides head-on with the dense energetic attosecond electron bunches, resulting in efficient emission of bright multi-MeV attosecond γ-ray pulses. The spatial distributions of the laser intensity for the incident pulse (b) and in-cone pulse (c). Density distributions of electrons (d) and γ-photons (e)^[64].

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表 1 当前实验中不同物理机制下激光驱动的X射线源和伽马射线源的性能比较

Table 1. Comparison of the performance of laser-driven X-ray and gamma-ray sources under different physical mechanisms in current experiments.

	Betatron^[48]	Compton^[35]	Bremsstrahlung^[49]
能量范围/MeV	~0.1	0.3—2.0	0.1—30.0
带宽/%	~100	33—60	~100
光子数	10⁸—10⁹	10⁷—10⁸	10⁸—10⁹
峰值亮度/ (photons·s^–1· mm^–2·mrad^–2· 0.1%BW^–1)	~10²³	~10²²	~10¹⁷
尺寸/μm	~5	~4	~100
脉宽/fs	~10	~10	~10⁴
发散角/mrad	~5	~4	~40

DownLoad: CSV

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Research progress of ultrabright γ-ray radiation and electron-positron pair production driven by extremely intense laser fields

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Corresponding author: Wang Wei-Min, weiminwang1@ruc.edu.cn ; Sheng Zheng-Ming, zmsheng@sjtu.edu.cn ;

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Research progress of ultrabright γ-ray radiation and electron-positron pair production driven by extremely intense laser fields

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Corresponding author: Wang Wei-Min, weiminwang1@ruc.edu.cn ; Sheng Zheng-Ming, zmsheng@sjtu.edu.cn ;

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