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中国物理学会期刊

真空虚拟阴极控制方法研究

Research on control methods of virtual cathode in a vacuum

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  • 基于已有的一维虚拟阴极理论模型,本研究进一步建立了真空虚拟阴极控制理论,并由此研发了一套完整的真空虚拟阴极控制系统。该控制系统可以通过调节阴极加热温度、饱和电子发射电流以及电子收集电流等参数,从而分别实现对真空虚拟阴极电势和宽度的准确控制。以钨阴极为研究对象,进一步的测试结果表明,在保持电子收集电流与饱和电子发射电流之比不变时,虚拟阴极电势会随着加热温度的增加而线性增大;在保持加热温度不变时,虚拟阴极电势会随着电子收集电流的增大呈对数减小。另一方面,在满足强虚拟阴极条件时,虚拟阴极宽度与加热温度的四分之三次方成正比,与电子收集电流的二分之一次方成反比,而与阴极材料属性无关。

     

    As an important physical phenomenon caused by thermionic emission, the virtual cathode not only has significant scientific research value, but also has broad application prospects. In our recent research, a one-dimensional model of thermionic emission was established, and the analytical expressions for the potential barrier and the spatial width of virtual cathodes were derived, which were of great significance for improving the understanding of virtual cathodes and developing methods to control the virtual cathode characteristics. In this study, based on the existing theoretical, we further establish a control theory of virtual cathodes and develop a complete virtual cathode control system accordingly. The hardware components of this control system mainly include a vacuum chamber, a hot-cathode filament, an anode, a capture card, a computer, a cathode heating circuit, a cathode scanning bias circuit, and an infrared temperature measurement system, etc. Using the control system, it is possible to achieve accurate control of the virtual cathode potential and width in a vacuum by adjusting parameters such as the cathode heating temperature and the electron collection current. Taking a tungsten filament as the research object, the virtual cathode potential and width generated by the tungsten cathode were measured and controlled respectively by using the method of controlling variables. The experimental results show that the virtual cathode potential increases linearly with the rising heating temperature when the ratio of electron collection current to saturated electron emission current is kept constant, and decreases logarithmically with the increase of the electron collection current when the heating temperature remains constant. On the other hand, when the strong virtual cathode condition is met, the virtual cathode width is proportional to the three-fourths power of the heating temperature, inversely proportional to the square root of the electron collection current, and is independent of the cathode material parameters.

     

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