Further Studies on Using the AHFP Exponent to Choose Between Alternative Field Emission Theories

Sergey Filippov, R. Forbes, E. O. Popov, A. G. Kolosko, F. F. Dall’Agnol
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引用次数: 1

Abstract

The general background to this research is set out in [1], [2]. It is based on the idea that an experimentally measured value of the so-called “AHFP exponent” kmight be used to choose between alternative theories of field electron emission (FE), in the first instance between 1928/29 Fowler-Nordheim (FN) FE theory and 1956 Murphy-Good (MG) FE theory. Amongst several factors that influence predicted theoretical ranges for x-values are the shape and local work function of a point-like or post-like field emitter. Our earlier work [1] explored a limited range of these parameters, but the overall conclusion was that the only x-value (1.63) considered adequately reliable did not yield a decisive result. As discussed in detail in this presentation, we have now explored a wider range of these parameters, but the outcome is still not a decisive result. Implications are discussed in a separate presentation [2].
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利用AHFP指数进行场发射理论选择的进一步研究
本研究的一般背景见[1],[2]。它基于这样一种想法,即所谓的“AHFP指数”k的实验测量值可用于在场电子发射(FE)的备选理论之间进行选择,首先是在1928/29年的Fowler-Nordheim (FN) FE理论和1956年的Murphy-Good (MG) FE理论之间进行选择。在影响x值预测理论范围的几个因素中,有点状或柱状场发射极的形状和局部功函数。我们早期的工作[1]探讨了这些参数的有限范围,但总体结论是,唯一被认为足够可靠的x值(1.63)并不能产生决定性的结果。正如本报告中详细讨论的那样,我们现在已经探索了这些参数的更大范围,但结果仍然不是决定性的结果。影响将在单独的报告中讨论[2]。
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