Abstract
The effectiveness of silicon surface passivation by \(\mathrm{Al}_{2}\mathrm{O}_{3}\) is fundamentally determined by the properties of the various electronic states present at the Si–Al\(_{2}\)O\(_{3}\) interface.
Unity of plan everywhere lies hidden under the mask: of diversity of structure—the complex is everywhere evolved out of the simple.
—Thomas Henry Huxley
A Lobster; or, the Study of Zoology
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Notes
- 1.
- 2.
Note that Tanaka and Iwauchi [36] used the tunnelling model of [37] to account for frequency dispersion, rather than the surface potential fluctuation model of [25] used here and in most recent works, resulting in a systematically larger value for \(\sigma _{n}\). The value of \(\sigma _{n}\) corresponding to the measurements of [36] is reassessed in Fig. 4.7.
- 3.
Each of the preceding authors used different values of \(v_{\textit{th}}\) in extracting \(\sigma _{\!p}\) and \(\sigma _{n}\), either \(2 \times 10^{7}\,\mathrm{cm}\,\mathrm{s}^{-1}\) [36], \(5 \times 10^{7}\,\mathrm{cm}\,\mathrm{s}^{-1}\) [38], or \(1 \times 10^{7}\,\mathrm{cm}\,\mathrm{s}^{-1}\) [32]. The values mentioned in the text have been normalised to \(v_{\textit{th}} = 2 \times 10^{7}\,\mathrm{cm}\,\mathrm{s}^{-1}\).
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Black, L.E. (2016). Electrical Properties of the Si–Al\(_{2}\)O\(_{3}\) Interface. In: New Perspectives on Surface Passivation: Understanding the Si-Al2O3 Interface. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-32521-7_4
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