压缩射频离子源的技术和物理方面

M. Aziz, F. Salam, M. Talat, A. Helal, H. El-Khabeary T., N.T. El-Merai
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摘要

给出了氮离子和氩离子在不同压力和射频功率下的性能实验结果。结果是采用压缩轴向射频离子源,出口孔径半径与提取间隙宽度的纵横比为0.4。我们的数据证实了当前标度定律在射频功率为50瓦和20瓦时的有效性,分别适用于氮气和氩气,压力为3 /spl mu/Hg。结果表明,随着压力的增大,束流电流会减小。因此,为了保持波束电流恒定,必须增加射频功率。以氮气为例,在0.24/spl倍/10/sup -8/安培/V/sup 3/2/对应的压力为0.03/spl倍/10/sup -8/安培/V/sup 3/2/对应的压力为25 /spl mu/Hg时,性能降至1.2/spl度/。以氩气为例,当性能为0.12/spl倍/10/sup -8/安培/V/sup 3/2/时,对应于3/ spl mu/Hg的压力,光束发散度为7.2/spl度;当性能为0.02/spl倍/10/sup -8/安培/V/sup 3/2/时,对应于25 /spl mu/Hg的压力,光束发散度为3.2。
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Technological and physical aspects of a constricted RF ion source
Experimental results are given for the perveance at different pressures and RF power using nitrogen and argon ions. The results are taken using a constricted axial RF ion source with an aspect ratio of the radius of the outlet aperture to the extraction gap width equals 0.4. Our data confirm the validity of the current scaling law at RF power equals 50 watt 20 watt in case of nitrogen and argon gases respectively at a pressure of 3 /spl mu/Hg. It is found that by increasing the pressure the beam current will decrease. Therefore, in order to keep the beam current constant, the RF power must be increased. In case of nitrogen, at a perveance of 0.24/spl times/10/sup -8/ Amp/V/sup 3/2/ corresponding to a pressure of 0.03/spl times/10/sup -8/ Amp/V/sup 3/2/ corresponding to a pressure of 25 /spl mu/Hg, it reduces to 1.2/spl deg/. In case of argon, at a perveance of 0.12/spl times/10/sup -8/ Amp/V/sup 3/2/ corresponding to a pressure of 3 /spl mu/Hg, the beam divergence is 7.2/spl deg/, while at a perveance of 0.02/spl times/10/sup -8/ Amp/V/sup 3/2/ corresponding to a pressure of 25 /spl mu/Hg, it becomes 3.2.
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