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- Q6822560 subject Q6947582.
- Q6822560 subject Q7662241.
- Q6822560 abstract "In bulk semiconductor band structure calculations, it is assumed that the crystal lattice (which features a periodic potential due to the atomic structure) of the material is infinite. When the finite size of a crystal is taken into account, the wavefunctions of electrons are altered and states that are forbidden within the bulk semiconductor gap are allowed at the surface. Similarly, when a metal is deposited onto a semiconductor (by thermal evaporation, for example), the wavefunction of an electron in the semiconductor must match that of an electron in the metal at the interface. Since the Fermi levels of the two materials must match at the interface, there exists gap states that decay deeper into the semiconductor.".
- Q6822560 thumbnail Diagram_of_band-bending_interfaces_between_two_different_metals_and_two_different_semiconductors.jpg?width=300.
- Q6822560 wikiPageWikiLink Q108193.
- Q6822560 wikiPageWikiLink Q11426.
- Q6822560 wikiPageWikiLink Q11456.
- Q6822560 wikiPageWikiLink Q13633683.
- Q6822560 wikiPageWikiLink Q1419397.
- Q6822560 wikiPageWikiLink Q15119237.
- Q6822560 wikiPageWikiLink Q171407.
- Q6822560 wikiPageWikiLink Q179467.
- Q6822560 wikiPageWikiLink Q1924839.
- Q6822560 wikiPageWikiLink Q215589.
- Q6822560 wikiPageWikiLink Q2225.
- Q6822560 wikiPageWikiLink Q230895.
- Q6822560 wikiPageWikiLink Q2362761.
- Q6822560 wikiPageWikiLink Q2391942.
- Q6822560 wikiPageWikiLink Q421416.
- Q6822560 wikiPageWikiLink Q422819.
- Q6822560 wikiPageWikiLink Q467463.
- Q6822560 wikiPageWikiLink Q579501.
- Q6822560 wikiPageWikiLink Q670.
- Q6822560 wikiPageWikiLink Q6947582.
- Q6822560 wikiPageWikiLink Q7662241.
- Q6822560 wikiPageWikiLink Q783800.
- Q6822560 wikiPageWikiLink Q78974.
- Q6822560 wikiPageWikiLink Q806380.
- Q6822560 wikiPageWikiLink Q807994.
- Q6822560 wikiPageWikiLink Q867.
- Q6822560 wikiPageWikiLink Q895901.
- Q6822560 wikiPageWikiLink Q897.
- Q6822560 comment "In bulk semiconductor band structure calculations, it is assumed that the crystal lattice (which features a periodic potential due to the atomic structure) of the material is infinite. When the finite size of a crystal is taken into account, the wavefunctions of electrons are altered and states that are forbidden within the bulk semiconductor gap are allowed at the surface.".
- Q6822560 label "Metal-induced gap states".
- Q6822560 depiction Diagram_of_band-bending_interfaces_between_two_different_metals_and_two_different_semiconductors.jpg.