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Theoretical study on the thickness of polycrystalline semiconductor multialkali photocathodes

机译:多晶半导体多铝基光电阴性厚度的理论研究

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Optimum thickness of polycrystalline semiconductor multialkali photocathodes is studied by the exponential attenuation rate of the radiation intensity and formulas for the quantum yield spectra and optical absorption coefficient of multialkali photocathodes. It has been found that if I$-$alpha$//I$-O$/ $GRT 0.4, photocathode optimum thickness D will be in excess of around 1000 angstroms and if I$-$alpha$//I$-O$/ increases further, D will tend to increase too, while photoelectrons excited by energetic photons will appear in the inner surface of the photocathode. Furthermore, D should be in the vicinity of 300 angstroms for the first kind of photocathode (S-20, S-20R, and S-25) and 900 angstroms for the second kind of photocathodes (new S-25, Varo, and LEP). It is suggested that the optimum photocathode thickness D be studied by the spectral response peaks of multialkali photocathodes. We came to the conclusion that photoelectron escape depth and incident wavelength tends to increase and along with it the optimum photocathode thickness. It has been calculated that the optimum thickness of multialkali photocathodes possessing good response in visible and infrared light must be in the vicinity of 1200 angstroms.
机译:通过辐射强度和量子屈服光谱的辐射强度和公式的指数衰减率研究了多晶半导体多铝基甘油光电阴极的最佳厚度和多铝基光电阴离子的光学吸收系数的指数衰减。有人发现,如果我$ - $ alpha $ // i $ -o $ / $ grt 0.4,光电阴极最佳厚度d将超过1000埃,如果我$ - $ apha $ // i $ -o价格进一步增加,D趋于增加,而精力充沛的光子激励的光电子将出现在光电阴极的内表面中。此外,D应该在300埃附近,用于第一种光电阴极(S-20,S-20R和S-25)和900埃的第二种光电阴极(新S-25,Varo和LEP) )。建议通过多铝基光电容器的光谱响应峰研究最佳光电阴极厚度D.我们得出结论,光电子逃逸深度和入射波长趋于增加,并且随之而来的最佳光电阴极厚度。已经计算出具有在可见光和红外光中具有良好反应的多铝基光电偶的最佳厚度必须位于1200埃附近。

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