“…Due to the Be in host lattice, the binding energy in BeZnO was significantly enhanced to 263 meV, which is rather important to realize exciton lasers with a low threshold. Besides the bandgap modulation, Be x Zn 1– x O with low Be content was found to be helpful in reducing the acceptor ionization energy and improving the stability of p-type ZnO. , Even though Be x Zn 1– x O has achieved such progress, two unexpected shortcomings impede its further applications: (1) the crystal quality of Be x Zn 1– x O deteriorates rapidly as the Be content increases because of the large lattice mismatch (ZnO: a = 0.325 nm, c = 0.525 nm; BeO: a = 0.27 nm, c = 0.43 nm); (2) Be can easily occupy the interstitial position of the lattice due to the small Be 2+ radius. − Additionally, according to the thermal stability investigation, Be atoms were observed to be easily diffused out from the host lattice, and as a result, the BeO second phase will be generated. , Alternatively, quaternary alloy Be x Mg y Zn 1– x – y O was proposed to further modulate the bandgap of ZnO, because it may have the chance to overcome the difficulties occuring in ternary alloy Be x Zn 1– x O and Mg x Zn 1– x O. − Recently, quaternary alloy Be x Mg y Zn 1– x – y O with low Be content and high Mg content was prepared to obtain the largest bandgap (5.14 eV) in wurtzite structure II–VI alloys . Due to the strong Be–O chemical bond, a small amount of Be plays a crucial role to stabilize the quaternary system.…”