1971
DOI: 10.1016/0029-554x(71)90013-9
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An empirical equation for the backscattering coefficient of electrons

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Cited by 133 publications
(41 citation statements)
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“…A Si detector of this thickness is able to fully stop electrons with energies up to ∼350 keV, while at the same time having a rather low sensitivity to γ radiation in comparison to a thicker Si detector or a highpurity Ge detector. Another advantage of using a Si detector is that the electron backscattering probability for Si is significantly lower than for Ge (by a factor of about 2.3 [46]). …”
Section: A Experimental Setupmentioning
confidence: 99%
“…A Si detector of this thickness is able to fully stop electrons with energies up to ∼350 keV, while at the same time having a rather low sensitivity to γ radiation in comparison to a thicker Si detector or a highpurity Ge detector. Another advantage of using a Si detector is that the electron backscattering probability for Si is significantly lower than for Ge (by a factor of about 2.3 [46]). …”
Section: A Experimental Setupmentioning
confidence: 99%
“…(29) (for the energy dependence) and Ref. (31) (for the angular dependence) by a factor of approximately 1.2.…”
Section: Electrons Backscattering Simulationsmentioning
confidence: 99%
“…These results are consistent with each other at less than 0.5% precision. As a cross-check to these simulations, a phenomenological model was also used to parametrize electron backscattering which was derived from electron backscattering studies on plastic scintillators [45,46] and modified to match the results of Martin et al [47].…”
Section: Electron Backscatteringmentioning
confidence: 99%