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.
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页数:7
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