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Incident angle dependence of secondary electron emission from carbon induced by swift H2+

机译:快速H2 +诱导的碳二次电子发射的入射角依赖性

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摘要

The incident angle dependence of secondary electron emission induced by a swift H2+ ion impinging on carbon is studied using the Monte Carlo method combined with the semiempirical theory. The relationships both between the electron emission yield and the project angle and between the statistics and the projectile angle are investigated. The results show that the backward electron emission yield deviates from the inverse cosine law, due to the effect of the valence electrons of H2+. The ratio of the forward electron emission yield to the backward electron emission yield at the inclining incidence is different from that at the normal incidence. The statistical distribution of electron emission is independent of the incident angle. The value of b, the deviation parameter from the Poisson distribution, increases with projectile energy.
机译:利用蒙特卡罗方法结合半经验理论研究了快速H 2+离子撞击碳引起的二次电子发射的入射角依赖性。研究了电子发射量与投射角之间的关系以及统计与投射角之间的关系。结果表明,由于H2 +价电子的作用,后向电子发射产率偏离反余弦定律。倾斜入射时的正向电子发射产率与反向电子发射率之比与法向入射时不同。电子发射的统计分布与入射角无关。 b的值(与泊松分布的偏差参数)随射弹能量的增加而增加。

著录项

  • 来源
    《中国物理:英文版》 |2005年第7期|1465-1470|共6页
  • 作者单位

    National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China;

    Applied Ion Beam Physics Laboratory, Institute of Modern Physics, Fudan University, Shanghai 200433, China;

    Applied Ion Beam Physics Laboratory, Institute of Modern Physics, Fudan University, Shanghai 200433, China;

    Applied Ion Beam Physics Laboratory, Institute of Modern Physics, Fudan University, Shanghai 200433, China;

    Applied Ion Beam Physics Laboratory, Institute of Modern Physics, Fudan University, Shanghai 200433, China;

  • 收录信息 中国科技论文与引文数据库(CSTPCD);
  • 原文格式 PDF
  • 正文语种 chi
  • 中图分类 物理学;
  • 关键词

    secondary electron emission; incidence angle; Monte-Carlo simulation; valence electron; statistical distribution;

    机译:二次电子发射入射角蒙特卡罗模拟价电子统计分布;
  • 入库时间 2024-01-06 16:33:00
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