Answers are grounded in this paper and cite their sources.
We have performed photoelectron spectroscopy of the clean GaP(110) surface, obtained by cleaving n-type specimens. The results show that Fermi-level stabilization occurs in a wide range of positions. In some cases nearly flat bands were obtained. The surface Fermi-level position in n-type GaP(110) is then due to extrinsic surface states, probably cleavage defects, as in the case of p-type samples. The density of these extrinsic states depends upon the quality of the cleave. Previously the Fermi-level pinning in n-type GaP(110) surfaces instead was attributed to (empty) intrinsic surface states located at 1.6±{}0.1 eV above the valence band. GaP(110) was considered an exception among III-V compounds, since in general atomic relaxation removes intrinsic surface states from the fundamental gap. The present results set a lower bound for the energetic position of the empty surface states slightly below the bottom of the conduction band. Therefore GaP(110) exhibits a gap practically free from intrinsic surface states, like the other III-V compounds so far investigated. We have also performed a spectroscopic study of the empty (intrinsic) surface states on the same surface by measuring the absorption edge of the P 2p core level. The result shows that the wave functions of the empty dangling-bond states, mainly cationic in origin, have a sizable localization on the anion site as well.
No takes yet. Share an insight, caveat, or question.
Chiaradia et al. (1989) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: