ABSTRACT A bilayer of V 0.49 N 0.51 /V 0.56 N 0.44 has been grown epitaxially on MgO(001) by reactive high‐power pulsed magnetron sputtering in an industrial‐scale deposition system at a temperature of 400°C, and it is demonstrated that the defect structure and interfacial strain are governed by the N concentration. Based on the lattice mismatch between MgO and V 0.49 N 0.51 with V vacancies, an interfacial strain of −2.3(1)% is expected. From ab initio calculations, X‐ray diffraction, and transmission electron microscopy data, it is inferred that the V 0.49 N 0.51 layer exhibits V vacancies, N Frenkel pairs, and a high dislocation density of ≈0.20 nm −2 , causing an interfacial strain of −1.4(5)% at the MgO/V 0.49 N 0.51 interface. The phase formation of understoichiometric V 0.56 N 0.44 is governed by N vacancy formation, while the dislocation density is reduced to ≈0.04 nm −2 at the V 0.49 N 0.51 /V 0.56 N 0.44 interface and to < 0.01 nm −2 within V 0.56 N 0.44 at a distance of ≈35 nm from the interface. Based on ab initio calculations, a strain of −1.7(6)% is predicted at the V 0.49 N 0.51 /V 0.56 N 0.44 interface in very good agreement with the experimentally obtained value of −1.6(8)%. It is evident that control of the N concentration allows for the design of layered architectures with well‐defined strained interfaces and tailored defect structures.
Hans et al. (Sun,) studied this question.