Dense electron-positron plasmas and gamma-ray bursts generation by counter-propagating quantum electrodynamics-strong laser interaction with solid targets

被引:54
|
作者
Luo, Wen [1 ,2 ]
Zhu, Yi-Bo [1 ]
Zhuo, Hong-Bin [3 ,4 ]
Ma, Yan-Yun [3 ,4 ]
Song, Ying-Ming [1 ]
Zhu, Zhi-Chao [1 ]
Wang, Xiao-Dong [1 ]
Li, Xing-Huo [3 ]
Turcu, I. C. E. [2 ]
Chen, Min [4 ,5 ,6 ]
机构
[1] Univ South China, Sch Nucl Sci & Technol, Hengyang 421001, Peoples R China
[2] Horia Hulubei Natl Inst R&D Phys & Nucl Engn IFIN, Extreme Light Infrastruct Nucl Phys ELI NP, RO-077125 Bucharest, Jud Ilfov, Romania
[3] Natl Univ Def Technol, Coll Sci, Changsha 410073, Hunan, Peoples R China
[4] Shanghai Jiao Tong Univ, IFSA Collaborat Innovat Ctr, Shanghai 200240, Peoples R China
[5] Shanghai Jiao Tong Univ, Minist Educ, Key Lab Laser Plasmas, Shanghai 200240, Peoples R China
[6] Shanghai Jiao Tong Univ, Dept Phys & Astron, Shanghai 200240, Peoples R China
基金
中国国家自然科学基金;
关键词
THOMSON SCATTERING; PAIR PRODUCTION; DRIVEN; ABSORPTION; PHYSICS; FIELD;
D O I
10.1063/1.4923265
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
We use quantum electrodynamics (QED) particle-in-cell simulations to investigate and compare the generation of dense electron-positron plasmas and intense c-ray bursts in the case of counter-propagating laser solid interaction (two-side irradiation) and single laser solid interaction (one-side irradiation). In the case of counter-propagating linearly polarized laser pulses irradiating a thin aluminum foil with each pulse peak power of 12.5 PW (I = 4 x 10(23) W/cm(2)), we calculate that about 20% of the laser energy is converted into a burst of gamma-rays with flux exceeding 10(14) s(-1) This would be one of the most intense c-ray sources among those currently available in laboratories. The c-ray conversion efficiency in the case of two-side irradiation is three times higher than in the case of one-side irradiation using a single 12.5 PW laser. Dense electron-positron plasma with a maximum density of 6 x 10(27) m(-3) are generated simultaneously during the two-side irradiation which is eightfold denser compared to the one-side irradiation. The enhancement of the effects in the case of counter-propagating lasers are the results of the symmetrical compression of the foil target and the formation of electric potential and standing wave around the target. Realizing experimentally the proposed counter-propagating QED-strong laser-solid interaction to produce dense electron-positron pairs and prolific c-rays will be made possible by the Extreme Light Infrastructure-Nuclear Physics facility under construction. (C) 2015 AIP Publishing LLC.
引用
收藏
页数:7
相关论文
共 3 条
  • [1] Dense electron-positron plasmas and bursts of gamma-rays from laser-generated quantum electrodynamic plasmas
    Ridgers, C. P.
    Brady, C. S.
    Duclous, R.
    Kirk, J. G.
    Bennett, K.
    Arber, T. D.
    Bell, A. R.
    PHYSICS OF PLASMAS, 2013, 20 (05)
  • [2] Resonant Production of High-Energy Electron-Positron Pairs and Gamma Quanta in the Quantum Electrodynamics Processes in Strong Laser Fields
    Roshchupkin, S. P.
    Dubov, V. V.
    Dubov, A., V
    Doroshenko, D., V
    Larin, N. R.
    Sizykh, G. K.
    Serov, V. D.
    HIGH POWER LASERS AND APPLICATIONS, 2021, 11777
  • [3] Generation of extreme-ultraviolet and x-ray light from a propagating nanometer electron layer in few-cycle laser interaction with solid targets
    Liu, Xinmeng
    Yue, Dongning
    Dong, Quanli
    Shao, Ziqiang
    Li, Zhe
    Teng, Hao
    Wei, Zhiyi
    Liu, Feng
    Li, Boyuan
    Yuan, Xiaohui
    Chen, Min
    Sheng, Zhengming
    Zhang, Jie
    PHYSICAL REVIEW A, 2024, 109 (04)