Формирование плазмы в атмосфере азота импульсным электронным пучком вблизи диэлектрической мишени при форвакуумных давлениях

Алексей Валерьевич Казаков, Е. М. Окс, Н.А. Панченко
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Abstract

Features of the processes of beam plasma formation near a dielectric (aluminum oxide ceramic) target being irradiated by an intense pulsed electron beam in the forevacuum pressure range (4–15 Pa) have been investigated. It has been established that the density of the beam plasma near the irradiated dielectric target is higher than in the case of "free" propagation of the electron beam. The observed increase in plasma density depends on the emission current (electron beam current), gas pressure, and accelerating voltage. The influence of the dielectric target on the beam plasma density is due to emission of electrons from the target surface and the uncompensated negative potential on the target surface, which determines the energy of emitted electrons. An increase in gas pressure leads to a smaller increase in the beam plasma density due to a decrease in the absolute value of the negative potential. Varying the electron beam current and accelerating voltage provide to control the beam plasma density.
在真空压力下,在氮气大气中等离子体形成
本文研究了在前真空压力范围(4 ~ 15pa)内,强脉冲电子束辐照介质(氧化铝陶瓷)靶附近束等离子体形成过程的特征。已经确定,在辐照介质目标附近的束等离子体密度高于电子束“自由”传播的情况。观察到的等离子体密度的增加取决于发射电流(电子束电流)、气体压力和加速电压。介质靶对束流等离子体密度的影响是由于靶表面的电子发射和靶表面未补偿的负电位决定了发射电子的能量。由于负电位的绝对值降低,气体压力的增加导致束等离子体密度的增加较小。通过改变电子束电流和加速电压来控制束流等离子体密度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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