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Anode plasma ionization due to sheath heating in magnetically insulated ion diodes

机译:磁绝缘离子二极管中由于护套加热而产生的阳极等离子体电离

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We show that anode plasma sheath heating can cause undesirableinsituionization of the anode plasma in magnetically insulated ion diodes. We find that extremely high electron energies will occur in the anode plasma sheath due to an increasing magnetic field at the anode surface during the diode pulse. These high‐energy electrons can collisionally ionize the plasma ions to an unwanted ionization state. Multiply ionized anode plasma ions represent a beam contaminant that may cause undesired preheat in inertial confinement fusion (ICF) capsules. The fraction of unwanted higher ionization states increases with anode plasma density. Therefore, this effect places an upper limit on the anode plasma density that can be used in an ICF application. As an example, we estimate the fraction of Li++generated by sheath heating in the PBFA‐II Applied‐Bion diode as a function of the initial Li+anode plasma density and obtain an upper limit for a lithium anode plasma density of approximately 1×1016cm−3. At anode plasma densities of 1×1016cm−3or less there will be substantial motion of the ion emitting surface during the diode pulse. We discuss the advantages and disadvantages of this plasma motion.
机译:我们表明,阳极等离子体护套加热会导致磁绝缘离子二极管中阳极等离子体的不良局部电离。我们发现,在二极管脉冲期间,由于阳极表面的磁场增加,阳极等离子体护套中会出现极高的电子能量。这些高能电子可以碰撞地将等离子体离子电离到不需要的电离状态。多重电离阳极等离子体离子代表一种束流污染物,可能导致惯性约束聚变 (ICF) 胶囊中出现不必要的预热。不需要的高电离态的比例随着阳极等离子体密度的增加而增加。因此,这种效应对可用于ICF应用的阳极等离子体密度设置了上限。例如,我们估计了PBFA&连字符II应用&连字符Bion 二极管中护套加热产生的Li++的比例作为初始Li+阳极等离子体密度的函数,并得到了锂阳极等离子体密度的上限约为1×1016cm−3。当阳极等离子体密度为1×1016cm−3或更小时,在二极管脉冲期间,离子发射表面将发生大量运动。我们讨论了这种等离子体运动的优缺点。

著录项

  • 来源
    《journal of applied physics》 |1987年第4期|1288-1296|共页
  • 作者

    Stephen A. Slutz;

  • 作者单位
  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 英语
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