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First-principles calculations of the II-VI semiconductor $\beta$-HgS: Metal or semiconductor
Relativistic all-electron full-potential first-principles calculations have been performed in order to study the symmetry of the energy levels around the valence band maximum in the zinc blende II-VI semiconductors $\beta$-HgS, HgSe, and HgTe. It is demonstrated that in general, an inverted band-str...
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Lenguaje: | eng |
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2002
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Acceso en línea: | http://cds.cern.ch/record/646471 |
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author | Delin, A |
author_facet | Delin, A |
author_sort | Delin, A |
collection | CERN |
description | Relativistic all-electron full-potential first-principles calculations have been performed in order to study the symmetry of the energy levels around the valence band maximum in the zinc blende II-VI semiconductors $\beta$-HgS, HgSe, and HgTe. It is demonstrated that in general, an inverted band-structure does not necessarily lead to a zero fundamental energy gap for systems with zinc blende symmetry. Specifically, $\beta$-HgS is found to have at the same time an inverted band structure, and a small, slightly indirect, fundamental energy gap. Possibly, the energy levels around the valence band maximum order differently in each of these systems. |
id | cern-646471 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2002 |
record_format | invenio |
spelling | cern-6464712019-09-30T06:29:59Zhttp://cds.cern.ch/record/646471engDelin, AFirst-principles calculations of the II-VI semiconductor $\beta$-HgS: Metal or semiconductorXXRelativistic all-electron full-potential first-principles calculations have been performed in order to study the symmetry of the energy levels around the valence band maximum in the zinc blende II-VI semiconductors $\beta$-HgS, HgSe, and HgTe. It is demonstrated that in general, an inverted band-structure does not necessarily lead to a zero fundamental energy gap for systems with zinc blende symmetry. Specifically, $\beta$-HgS is found to have at the same time an inverted band structure, and a small, slightly indirect, fundamental energy gap. Possibly, the energy levels around the valence band maximum order differently in each of these systems.IC-2002-40oai:cds.cern.ch:6464712002 |
spellingShingle | XX Delin, A First-principles calculations of the II-VI semiconductor $\beta$-HgS: Metal or semiconductor |
title | First-principles calculations of the II-VI semiconductor $\beta$-HgS: Metal or semiconductor |
title_full | First-principles calculations of the II-VI semiconductor $\beta$-HgS: Metal or semiconductor |
title_fullStr | First-principles calculations of the II-VI semiconductor $\beta$-HgS: Metal or semiconductor |
title_full_unstemmed | First-principles calculations of the II-VI semiconductor $\beta$-HgS: Metal or semiconductor |
title_short | First-principles calculations of the II-VI semiconductor $\beta$-HgS: Metal or semiconductor |
title_sort | first-principles calculations of the ii-vi semiconductor $\beta$-hgs: metal or semiconductor |
topic | XX |
url | http://cds.cern.ch/record/646471 |
work_keys_str_mv | AT delina firstprinciplescalculationsoftheiivisemiconductorbetahgsmetalorsemiconductor |