Electronic structure at interfaces of cubic Gd2O3 with embedded Si nanocrystals

Research output: Contribution to journalArticleResearchpeer review

Authors

  • M. Badylevich
  • S. Shamuilia
  • V. V. Afanas'ev
  • A. Stesmans
  • A. Laha
  • H. J. Osten
  • A. Fissel

External Research Organisations

  • KU Leuven
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Details

Original languageEnglish
Pages (from-to)2382-2384
Number of pages3
JournalMicroelectronic engineering
Volume85
Issue number12
Early online date12 Sept 2008
Publication statusPublished - Dec 2008

Abstract

The electronic structure of silicon nanocrystals (∼2-6 nm in size) embedded in cubic Gd2O3 epi-layers grown on (1 1 1) Si was analyzed using spectroscopic ellipsometry and photocharging methods. With decreasing nanocrystal size down to the 2 nm range, the optical absorption exhibits a spectacular shift in spectral threshold to 2.9 ± 0.1 eV, as compared to the 1.12 eV absorption edge of the bulk Si crystal. This shift suggests a significant influence of quantum confinement on the Si nanocrystal/oxide interface band diagram, which effect is shown to be predominantly caused by an upshift of the nanocrystal conduction band.

Keywords

    Band alignment, Bandgap width, Insulator, Nanocrystals

ASJC Scopus subject areas

Cite this

Electronic structure at interfaces of cubic Gd2O3 with embedded Si nanocrystals. / Badylevich, M.; Shamuilia, S.; Afanas'ev, V. V. et al.
In: Microelectronic engineering, Vol. 85, No. 12, 12.2008, p. 2382-2384.

Research output: Contribution to journalArticleResearchpeer review

Badylevich, M, Shamuilia, S, Afanas'ev, VV, Stesmans, A, Laha, A, Osten, HJ & Fissel, A 2008, 'Electronic structure at interfaces of cubic Gd2O3 with embedded Si nanocrystals', Microelectronic engineering, vol. 85, no. 12, pp. 2382-2384. https://doi.org/10.1016/j.mee.2008.09.002
Badylevich, M., Shamuilia, S., Afanas'ev, V. V., Stesmans, A., Laha, A., Osten, H. J., & Fissel, A. (2008). Electronic structure at interfaces of cubic Gd2O3 with embedded Si nanocrystals. Microelectronic engineering, 85(12), 2382-2384. https://doi.org/10.1016/j.mee.2008.09.002
Badylevich M, Shamuilia S, Afanas'ev VV, Stesmans A, Laha A, Osten HJ et al. Electronic structure at interfaces of cubic Gd2O3 with embedded Si nanocrystals. Microelectronic engineering. 2008 Dec;85(12):2382-2384. Epub 2008 Sept 12. doi: 10.1016/j.mee.2008.09.002
Badylevich, M. ; Shamuilia, S. ; Afanas'ev, V. V. et al. / Electronic structure at interfaces of cubic Gd2O3 with embedded Si nanocrystals. In: Microelectronic engineering. 2008 ; Vol. 85, No. 12. pp. 2382-2384.
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title = "Electronic structure at interfaces of cubic Gd2O3 with embedded Si nanocrystals",
abstract = "The electronic structure of silicon nanocrystals (∼2-6 nm in size) embedded in cubic Gd2O3 epi-layers grown on (1 1 1) Si was analyzed using spectroscopic ellipsometry and photocharging methods. With decreasing nanocrystal size down to the 2 nm range, the optical absorption exhibits a spectacular shift in spectral threshold to 2.9 ± 0.1 eV, as compared to the 1.12 eV absorption edge of the bulk Si crystal. This shift suggests a significant influence of quantum confinement on the Si nanocrystal/oxide interface band diagram, which effect is shown to be predominantly caused by an upshift of the nanocrystal conduction band.",
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T1 - Electronic structure at interfaces of cubic Gd2O3 with embedded Si nanocrystals

AU - Badylevich, M.

AU - Shamuilia, S.

AU - Afanas'ev, V. V.

AU - Stesmans, A.

AU - Laha, A.

AU - Osten, H. J.

AU - Fissel, A.

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AB - The electronic structure of silicon nanocrystals (∼2-6 nm in size) embedded in cubic Gd2O3 epi-layers grown on (1 1 1) Si was analyzed using spectroscopic ellipsometry and photocharging methods. With decreasing nanocrystal size down to the 2 nm range, the optical absorption exhibits a spectacular shift in spectral threshold to 2.9 ± 0.1 eV, as compared to the 1.12 eV absorption edge of the bulk Si crystal. This shift suggests a significant influence of quantum confinement on the Si nanocrystal/oxide interface band diagram, which effect is shown to be predominantly caused by an upshift of the nanocrystal conduction band.

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