The electronic properties of hydrogenated, spherical
SiGe and GeSi
core–shell nanocrystals, with a diameter ranging from 1.8 to
4.0 nm, are studied within density functional theory. Effects induced
by quantum confinement and strain on the near-band-edge state localization,
as well as the band-offset properties between Si and Ge regions, are
investigated in detail. On the one hand, we prove that SiGe core–shell
nanocrystals always show a type II band-offset alignment, with the
HOMO mainly localized on the Ge shell region and the LUMO mainly localized
on the Si core region. On the other hand, our results point out that
a type II offset cannot be observed in small (diameter less than 3
nm) GeSi core–shell nanocrystals. In these systems, quantum
confinement and strain drive the near-band-edge states to be mainly
localized on Ge atoms, i.e., in the core region. In larger GeSi core–shell
nanocrystals, instead, the formation of a type II offset can be engineered
by playing with both core and shell thickness. The factors which determine
the band-offset character at the Ge/Si interface are discussed in
detail.