4.5 Article

Emission of the backscattered electron in the energy range of 20 to100 keV

Journal

ANNALS OF NUCLEAR ENERGY
Volume 196, Issue -, Pages -

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.anucene.2023.110230

Keywords

Backscattered electrons emission; Metal films; Backscattering coefficient; Molybdenum; Tungsten; Mean value of maximum penetration depth of; emitted backscattered electrons; Maximum penetration depth distribution of

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This paper presents a theoretical model for backscattered electron emission (BEE) and derives universal formulas for certain parameters within a specific energy range. These formulas can be used to calculate the backscattering coefficient and the maximum penetration depth distribution of backscattered electrons for different metals.
This paper presented the theoretical model of backscattered electron emission BEE, and the universal formulas for some parameters such as ri(h, Epo, Z) andf(x, Epo, Z) at Epo = 20-100 keV were deduced, respectively; where Epo is the incident energy of primary electron,f(x, Epo, Z) is maximum penetration depth distribution of emitted backscattered electron BE from atomic number Z bulk metals penetrated by primary electrons at Epo, x is the distance from incident surface to the position where primary electrons are reflected back, ri(h, Epo, Z) is the backscattering coefficient at Epo of Z metal films with film thickness h. From the deduced universal formula for ri(h, Epo, Z) and the relationships among the parameters of BEE from Au, W, Ag and Mo, the special formulas for some parameters such as ri(h, Epo, Z) andf(x, Epo, Z) of W and Mo were also obtained and proved correct, respectively.

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