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Jianxun LIU (刘建勋), Yanyun MA (马燕云), Xiaohu YANG (杨晓虎), Jun ZHAO (赵军), Tongpu YU (余同普), Fuqiu SHAO (邵福球), Hongbin ZHUO (卓红斌), Longfei GAN (甘龙飞), Guobo ZHANG (张国博), Yuan ZHAO (赵媛), Jingkang YANG (杨靖康). High-energy-density electron beam generation in ultra intense laser-plasma interaction[J]. Plasma Science and Technology, 2017, 19(1): 15001-015001. DOI: 10.1088/1009-0630/19/1/015001
Citation: Jianxun LIU (刘建勋), Yanyun MA (马燕云), Xiaohu YANG (杨晓虎), Jun ZHAO (赵军), Tongpu YU (余同普), Fuqiu SHAO (邵福球), Hongbin ZHUO (卓红斌), Longfei GAN (甘龙飞), Guobo ZHANG (张国博), Yuan ZHAO (赵媛), Jingkang YANG (杨靖康). High-energy-density electron beam generation in ultra intense laser-plasma interaction[J]. Plasma Science and Technology, 2017, 19(1): 15001-015001. DOI: 10.1088/1009-0630/19/1/015001
  • By using a two-dimensional particle-in-cell simulation, we demonstrate a scheme for high-energy-density electron beam generation by irradiating an ultra intense laser pulse onto an aluminum (Al) target. With the laser having a peak intensity of 4×1023 Wcm−2, a high quality electron beam with a maximum density of 117nc and a kinetic energy density up to 8.79×1018 Jm−3 is generated. The temperature of the electron beam can be 416 MeV, and the beam divergence is only 7.25°. As the laser peak intensity increases (e.g., 1024 Wcm−2), both the beam energy density (3.56×1019 Jm−3) and the temperature (545 MeV) are increased, and the beam collimation is well controlled. The maximum density of the electron beam can even reach 180nc. Such beams should have potential applications in the areas of antiparticle generation, laboratory astrophysics, etc.
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