We propose the Zn2V(1–x)Nb
x
N3 alloy
as a new
promising material for optoelectronic applications, in particular
for light-emitting diodes (LEDs). We perform accurate electronic-structure
calculations of the alloy for several concentrations x using density-functional theory with meta-GGA exchange–correlation
functional TB09. The band gap is found to vary between 2.2 and 2.9
eV with varying V/Nb concentration. This range is suitable for developing
bright LEDs with tunable band gap as potential replacements for the
more expensive Ga(1–x)In(x)N systems. Effects of configurational disorder are
taken into account by explicitly considering all possible distributions
of the metal ions within the metal sublattice for the chosen supercells.
We have evaluated the band gap’s nonlinear behavior (bowing)
with variation of V/Nb concentration for two possible scenarios:
(i) only the structure with the lowest total energy is present at
each concentration and (ii) the structure with minimum band gap is
present at each concentration, which corresponds to experimental conditions
when also metastable structures are presents. We found that the bowing
is about twice larger in the latter case. However, in both cases,
the bowing parameter is found to be lower than 1 eV, which is about
twice smaller than that in the widely used Ga(1–x)In(x)N alloy. Furthermore,
we found that both crystal volume changes due to alloying and local
effects (atomic relaxation and the V–N/Nb–N bonding
difference) have important contributions to the band gap bowing in
Zn2V(1–x)Nb
x
N3.