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Special features of plasma generation and beam formation for fore-vacuum plasma electron sources

机译:前真空等离子体电子源等离子体生成和梁形成的特点

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The paper reviews results of further development and applications of so called fore-vacuum plasma electron sources. The fore-vacuum pressure plasma-cathode electron sources provide efficient generation of continuous and pulsed electron beams in the otherwise inaccessible pressure range from several Pa to about one hundred Pa. Interest in the generation of electron beams at fore-vacuum pressures is dominated by the possibility of their use for surface treatment of dielectric (insulating) materials, ceramics, polymers and some others. This kind of e-beam sources utilizes either a hollow-cathode glow discharge or a cathodic arc discharge for formation of emission plasmas. Arc is mainly used for pulsed mode of electron source operation. Transition of hollow cathode glow to cathodic arc, with its associated cathode spots, follows from the need to increase the electron beam current. The papers presents some of the characteristics and parameters of a pulsed cathodic arc discharge as configured for use in a forevacuum-pressure plasma-cathode electron source for the generation of broad electron beams. Main goal of such research was achievement an uniform distribution of electron beam current density. Another subject to report is demonstration the possibility to obtain homogeneous dense beam plasma in a closed dielectric cavity using a dc forevacuum plasma electron source based on hollow cathode glow. At optimum electron energy and gas pressure, the plasma density distribution lengthwise the cavity is inhomogeneous to no more than 10 %.
机译:纸质评价进一步发展和所谓的前真空等离子体电子来源的应用结果。前真空压等离子体阴极电子源在其他PA到约一百PA的其他不可访问的压力范围内提供有效的连续和脉冲电子束。在前真空压力下产生电子束的兴趣由它们用于介电(绝缘)材料,陶瓷,聚合物和其他一些表面处理的可能性。这种电子束源利用空心阴极辉光放电或用于形成排放等离子体的阴极电弧放电。电弧主要用于电子源操作的脉冲模式。从需要增加电子束电流的情况下,空心阴极光发出到阴极弧的转变。这些纸张介绍了脉冲阴极电弧放电的一些特性和参数,如图所示用于用于产生宽电子束的前气压等离子体阴极电子源。这种研究的主要目标是实现电子束电流密度均匀分布。报告的另一个主题是使用基于空心阴极光发光的DC Forevuum电子源在闭合介电腔中获得均匀密集束等离子体的可能性。在最佳电子能量和气体压力下,距离腔体的等离子体密度分布不​​均匀至于10%。

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