1979
DOI: 10.1103/physreva.19.557
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Doubly differential cross sections of secondary electrons ejected from gases by electron impact: 50-300 eV on helium

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Cited by 65 publications
(43 citation statements)
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“…Figure 2 shows the DDCS results of He. The DDCS results are found to be in good agreement with the experimental data of Sharp et al [2] for 55 eV impact and 10 eV ejected energy.…”
Section: Resultssupporting
confidence: 81%
“…Figure 2 shows the DDCS results of He. The DDCS results are found to be in good agreement with the experimental data of Sharp et al [2] for 55 eV impact and 10 eV ejected energy.…”
Section: Resultssupporting
confidence: 81%
“…In the past, several groups of experimentalists, namely Opal et al [1,2], Oda et al [3,4], Rudd et al [5,6], Shyn et al [7][8][9][10][11], Goruganthu et al [ 12] and Mfiller-Fiedler et al [13] obtained results for DDCS mainly for helium atom, because of the simple reason that it is the simplest atom for which experimental difficulties can be minimized. Unfortunately the results of the experiments of one group usually differ widely from those of other groups (see [14]).…”
Section: Introductionmentioning
confidence: 99%
“…Here, however, we are interested in maximizing the cross-section for generating low energy secondary electrons rather than the total ionization cross section. In fact, since the threshold ionization for helium is ∼ 24.58 eV, it is not surprising that the low energy cross-section peaks at E p ∼ 30 eV [100,101]. The incoming electron energy should therefore be set to around 30 eV, resulting in an optimal cross section of σ ion ∼ 0.05Å 2 for secondary electrons with energy below 1 eV [100].…”
Section: Low Energy Electron Sourcementioning
confidence: 99%