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基于Z-FDTD的THz波与等离子体相互作用

伍习光 胡洋 王平 南琳

伍习光, 胡洋, 王平, 等. 基于Z-FDTD的THz波与等离子体相互作用[J]. 强激光与粒子束, 2018, 30: 043102. doi: 10.11884/HPLPB201830.170309
引用本文: 伍习光, 胡洋, 王平, 等. 基于Z-FDTD的THz波与等离子体相互作用[J]. 强激光与粒子束, 2018, 30: 043102. doi: 10.11884/HPLPB201830.170309
Wu Xiguang, Hu Yang, Wang Ping, et al. Interaction of Terahertz wave with plasma based on Z-FDTD[J]. High Power Laser and Particle Beams, 2018, 30: 043102. doi: 10.11884/HPLPB201830.170309
Citation: Wu Xiguang, Hu Yang, Wang Ping, et al. Interaction of Terahertz wave with plasma based on Z-FDTD[J]. High Power Laser and Particle Beams, 2018, 30: 043102. doi: 10.11884/HPLPB201830.170309

基于Z-FDTD的THz波与等离子体相互作用

doi: 10.11884/HPLPB201830.170309
详细信息
    作者简介:

    伍习光(1993-), 男,硕士,从事电离层空间探测研究;wxgsgdsg3@163.com

  • 中图分类号: O53

Interaction of Terahertz wave with plasma based on Z-FDTD

  • 摘要: 利用Z变换时域有限差分法(Z-FDTD)计算等离子体鞘层中太赫兹(THz)波的传输特性,得出太赫兹波的功率反射和透射系数在等离子鞘层中随电磁波频率的变化曲线图,分析了太赫兹波的传输特性与等离子体结构参数(鞘层厚度、碰撞频率以及电子密度)的关系,对利用太赫兹波缓解等离子体鞘层通信中出现的“黑障”现象做了探讨。结果表明:太赫兹波能改善等离子体鞘层通信,为解决“黑障”问题提供了有效途径。
  • 图  1  一维等离子体计算模型

    Figure  1.  One dimensional plasma calculation model

    图  2  一维FDTD中场分量差分迭代

    Figure  2.  Difference iteration of field component in one-dimensional FDTD

    图  3  入射波电场强度

    Figure  3.  Amplitude of electric field intensity of incident wave

    图  4  入射波频谱

    Figure  4.  Spectrum of incident wave

    图  5  不同碰撞频率下的反射系数

    Figure  5.  Reflection coefficients at different collision frequencies

    图  6  不同碰撞频率下的透射系数

    Figure  6.  Transmission coefficients at different collision frequencies

    图  7  不同电子密度下的反射系数

    Figure  7.  Reflection coefficients at different electron density

    图  8  不同电子密度下的透射系数

    Figure  8.  Transmission coefficients at different electron density

    图  9  不同等离子体厚度下的反射系数等离子体(电子密度为1021 m-3)

    Figure  9.  Reflection coefficients at different plasma thickness (electron density is 1021 m-3)

    图  10  不同等离子体厚度下的透射系数等离子体(电子密度为1021 m-3)

    Figure  10.  Transmission coefficients at different plasma thickness (electron density is 1021 m-3)

    图  11  不同等离子体厚度下的反射系数等离子体(电子密度为1020 m-3)

    Figure  11.  Reflection coefficients at different plasma thickness (electron density is 1020 m-3)

    图  12  不同等离子体厚度下的透射系数等离子体(电子密度为1020 m-3)

    Figure  12.  Transmission coefficients at different plasma thickness (electron density is 1020 m-3)

    图  13  不同等离子体碰撞频率下的反射系数

    Figure  13.  Reflection coefficients at different collision frequencies

    图  14  不同等离子体碰撞频率下的透射系数

    Figure  14.  Transmission coefficients at different collision frequencies

    图  15  不同等离子体厚度下的反射系数

    Figure  15.  Reflection coefficients at different plasma thickness inhomogeneous plasma

    图  16  不同等离子体厚度下的透射系数

    Figure  16.  Transmission coefficients at different plasma thickness inhomogeneous plasma

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出版历程
  • 收稿日期:  2017-08-08
  • 修回日期:  2017-11-23
  • 刊出日期:  2018-04-15

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