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氢原子束在大气长程传输中自剥离效应研究

沈硕 郝建红 张芳 赵强 范杰清 董志伟

沈硕, 郝建红, 张芳, 等. 氢原子束在大气长程传输中自剥离效应研究[J]. 强激光与粒子束, 2022, 34: 064004. doi: 10.11884/HPLPB202234.210481
引用本文: 沈硕, 郝建红, 张芳, 等. 氢原子束在大气长程传输中自剥离效应研究[J]. 强激光与粒子束, 2022, 34: 064004. doi: 10.11884/HPLPB202234.210481
Shen Shuo, Hao Jianhong, Zhang Fang, et al. Study on beam-induced-stripping effect of hydrogen atom beam in long distance propagation in atmosphere[J]. High Power Laser and Particle Beams, 2022, 34: 064004. doi: 10.11884/HPLPB202234.210481
Citation: Shen Shuo, Hao Jianhong, Zhang Fang, et al. Study on beam-induced-stripping effect of hydrogen atom beam in long distance propagation in atmosphere[J]. High Power Laser and Particle Beams, 2022, 34: 064004. doi: 10.11884/HPLPB202234.210481

氢原子束在大气长程传输中自剥离效应研究

doi: 10.11884/HPLPB202234.210481
基金项目: 高功率微波技术重点实验室基金项目(6142605200301); 国家自然科学基金委员会与中国工程物理研究院联合基金项目(U1730247)
详细信息
    作者简介:

    沈 硕,530802944@qq.com

    通讯作者:

    张 芳,zhang_fang@iapcm.ac.cn

  • 中图分类号: O46

Study on beam-induced-stripping effect of hydrogen atom beam in long distance propagation in atmosphere

  • 摘要: 氢原子束在大气传输时,束流粒子与大气粒子碰撞电离形成的大气剥离效应,以及和大气剥离产生次级粒子碰撞电离形成的自剥离效应,是造成氢原子束能量损失的重要机制。考虑到自剥离效应成因复杂,虽然目前已有一些理论方面的研究结果,但对其发生机理和对束流损失效果尚未有实验或数值模拟方面的工作,因此,通过对自剥离效应的发生机理和对束流损失的影响进行分析,进一步完善了自剥离效应理论,在通过束流传输方程验证了粒子云网格-蒙特卡罗法对氢原子束大气传输仿真模拟适用的基础上,将仿真结果与自剥离理论进行了对比,验证了自剥离效应理论的适用性。模拟结果表明,自剥离效应是由束流被大气电离产生的带电次级粒子团在地磁场的影响不停地穿越束流导致的,且自剥离效应的强弱与原子束的密度有关,束流密度越大,自剥离效应越强,对束流的影响越大。
  • 图  1  在不考虑自剥离时PIC-MCC模拟结果与束流传输方程对比

    Figure  1.  Comparison between PIC-MCC simulation results and beam propagation equation without considering self-stripping

    图  2  考虑自剥离时PIC-MCC模拟结果与束流传输方程对比

    Figure  2.  Comparison between PIC-MCC simulation results and beam propagation equation with considering self-stripping

    图  3  氢原子束大气传输模型示意

    Figure  3.  Schematic diagram of atmospheric transport model of hydrogen atom beam

    图  4  氢原子束极化电场

    Figure  4.  Polarization electric field of hydrogen atom beam

    图  5  密度为1.0×1018 m−3氢原子束大气传输时部分粒子的位置分布

    Figure  5.  Beam-induced stripping (BIS) products of hydrogen atomic beam (H-beam density 1.0×1018 m−3) propagating in atmosphere under the influence of geomagnetic field

    图  6  密度为1.0×1017 m−3氢原子束大气传输时部分粒子的位置分布

    Figure  6.  BIS products of hydrogen atomic beam (H-beam density 1.0×1017 m−3) propagating in atmosphere under the influence of geomagnetic field

    图  7  电子自剥离产生的次级粒子与氢离子自剥离产生的次级粒子的数量比

    Figure  7.  The ratio of the number of secondary particles produced by electron self-stripping to that produced by hydrogen ion self-stripping

    图  8  不同种类次级粒子自剥离效果对比

    Figure  8.  Comparison of BIS effect of different kinds of secondary particles

    图  9  不同初始束密度时束密度随传输距离的变化

    Figure  9.  Variation of beam density with transmission distance at different initial beam density

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出版历程
  • 收稿日期:  2021-11-04
  • 修回日期:  2022-02-26
  • 网络出版日期:  2022-03-11
  • 刊出日期:  2022-06-15

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