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Enhancement of high-charge-state ions in vacuum arc ion sources

机译:真空电弧离子源中高电荷态离子的增强

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Vacuum arc ion sources are used to generate high current broad beams of metal ions. The attraction of increasing the mean ion charge state in the beam is because of the possibility of thereby increasing the ion beam energy without applying higher extraction voltage. This is important both for heavy ion accelerator injectors and for ion implantation technologies. We have explored three different methods to enhance the degree of multiple ionization in vacuum arc plasmas. These methods are: application of a strong axial magnetic field in the arc region, generation of current spikes, and injected electron beam. A strong magnetic field increases the arc burning voltage because of improved confinement of the plasma column and leads to higher plasma electron temperature, which is primarily responsible for ionization. The B-field also increases the length of the ionization zone, beyond which there is no significant change in the ion charge state distribution (the distribution is frozen). Another approach to increase the arc voltage and electron temperature is to use an arc current spike of pulse duration comparable to the arc current relaxation time or less. This leads to a somewhat elevated arc voltage during the spike. Finally, additional ionization in the vacuum arc plasma can be brought about by injection into the plasma of an externally-produced electron beam. In this case the most important problem is to obtain optimum electron beam parameters and e-beam transport through the entire arc region. Here we describe these approaches and the experimental results of our investigations of ion charge state distribution. Mean ion charge states are presented, compared and discussed.
机译:真空电弧离子源用于产生大电流的金属离子宽束。增加离子束中平均离子电荷状态的吸引力是因为有可能在不施加较高提取电压的情况下增加离子束能量。这对于重型离子加速器注入器和离子注入技术都非常重要。我们已经探索了三种不同的方法来增强真空电弧等离子体中的多重电离度。这些方法是:在电弧区域中施加强轴向磁场,产生电流尖峰和注入电子束。由于改善了等离子体柱的限制,强磁场会增加电弧燃烧电压,并导致较高的等离子体电子温度,这主要是造成电离的原因。 B场还会增加电离区的长度,在此范围之外,离子电荷状态分布没有明显变化(该分布被冻结)。增加电弧电压和电子温度的另一种方法是使用脉冲持续时间与电弧电流弛豫时间或更短的电弧电流尖峰。这会导致在尖峰期间电弧电压有所升高。最后,通过将外部产生的电子束注入到等离子体中,可以在真空电弧等离子体中引起额外的电离。在这种情况下,最重要的问题是获得在整个电弧区域内的最佳电子束参数和电子束传输。在这里,我们描述了这些方法以及我们对离子电荷状态分布的研究的实验结果。给出,比较和讨论了平均离子电荷状态。

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