Band gaps and electron affinities of binary
and ternary, wurtzite (wz-) and zincblende (zb-) III-nitrides are
investigated using a unified hybrid density functional theory, and
band offsets between wz- and zb- alloys are calculated using Anderson’s
electron affinity model. A conduction (and valence) band offset of
1.85 (0.89) eV has been calculated for zb-GaN/InN heterojunctions,
which is 0.25 eV larger (and 0.26 eV smaller) than that of the wz-
counterpart. Such polarization-free zb-GaN/InGaN/GaN quantum well
structures with large conduction band offsets have the potential to
suppress electron leakage current and quantum-confined Stark effects
(QCSEs). Contrarily, the conduction (and valence) band offset of zb-AlN/GaN
heterojunctions is calculated to be 1.32 (0.43) eV, which is 1.15
eV smaller (and 0.13 eV larger) than that of the wz- case. The significant
reduction in zb-AlN/GaN band offsets is ascribed to the smaller and
indirect band gap of zb-AlNthe direct-to-indirect crossover
point in zb-Al
X
Ga1–X
N is when X ∼ 65%. The small
band gap of the zb-AlN barrier and the small conduction band offsets
imply that electrons can be injected into zb-AlN/GaN/AlN quantum well
heterostructures with small bias and less energy loss when captured
by the quantum wells, respectively, i.e., loss as heat is reduced.
The band gap of ternary III-nitrides does not linearly depend on alloy
compositions, implying a nonlinear dependence of band offsets on compositions.
As a result, the large bowing of the conduction band offset is identified
and ascribed to the cation-like behavior of the conduction band minimum,
while the linear dependence of the valence band offset on compositions
is attributed to the anion-like character of the valence band maximum.