Sub-TeV proton beam generation by ultra-intense laser irradiation of foil-and-gas target

被引:29
|
作者
Zheng, F. L. [1 ,2 ]
Wang, H. Y. [1 ]
Yan, X. Q. [1 ]
Tajima, T. [3 ]
Yu, M. Y. [4 ,5 ]
He, X. T. [1 ,6 ]
机构
[1] Peking Univ, Key Lab HEDP, Minist Educ, CAPT,State Key Lab Nucl Phys & Technol, Beijing 100871, Peoples R China
[2] China Acad Engn Phys, Grad Sch, Beijing 100088, Peoples R China
[3] LMU Munchen, Fak Phys, D-85748 Garching, Germany
[4] Zhejiang Univ, Inst Fus Theory & Simulat, Hangzhou 310027, Zhejiang, Peoples R China
[5] Ruhr Univ Bochum, Inst Theoret Phys 1, D-44780 Bochum, Germany
[6] Inst Appl Phys & Computat Math, Beijing 100088, Peoples R China
关键词
PLASMA-WAVES; ACCELERATION; FIELDS;
D O I
10.1063/1.3684658
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
A two-phase proton acceleration scheme using an ultra-intense laser pulse irradiating a proton foil with a tenuous heavier-ion plasma behind it is presented. The foil electrons are compressed and pushed out as a thin dense layer by the radiation pressure and propagate in the plasma behind at near the light speed. The protons are in turn accelerated by the resulting space-charge field and also enter the backside plasma, but without the formation of a quasistationary double layer. The electron layer is rapidly weakened by the space-charge field. However, the laser pulse originally behind it now snowplows the backside-plasma electrons and creates an intense electrostatic wakefield. The latter can stably trap and accelerate the pre-accelerated proton layer there for a very long distance and thus to very high energies. The two-phase scheme is verified by particle-in-cell simulations and analytical modeling, which also suggests that a 0.54 TeV proton beam can be obtained with a 10(23) W/cm(2) laser pulse. (C) 2012 American Institute of Physics. [doi:10.1063/1.3684658]
引用
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页数:5
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