Applying k -resolved inverse photoemission (KRIPES) to the √3×√3 R30°-reconstructed 6H-SiC(0001) face, we have observed a sharp surface state U located at 1.10 ± 0.05 eV above the Fermi level at the centre of the surface Brillouin zone. Its bandwidth of 0.34 ± 0.05 eV is in good agreement with the 0.35 eV predicted by first-principle calculations based on a Si-adatom model. However, LDA calculations predict a half-filled Σ 1 state and a metallic character for this reconstruction. Together with recent ARUPS data, our results reveal that the one-electron band Σ 1 is split into two bands, giving a semiconducting surface with a reduced indirect bandgap around 2.0 eV at the ′ point. Many-body correlation effects may give rise, in the limit of strong localization, to this bandgap opening.
No takes yet. Share an insight, caveat, or question.
Themlin et al. (1997) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: