Ab-initio DFT-FP-LAPW/TB-mBJ/LDA-GGA investigation of structural and electronic properties of MgxZn1−xO alloys in Würtzite, Rocksalt and Zinc-Blende phases. (September 2017)

• Record Type: Journal Article
• Authors: Djelal, A.; Chaibi, K.; Tari, N.; Zitouni, K.; Kadri, A.
• Is Part Of: Superlattices and microstructures. Volume 109(2017)
• Page Start: 81
• Page End: 98
• Publication Date: 2017-09
• Subjects: Superlattices as materials -- Periodicals; Microstructure -- Periodicals; Semiconductors -- Periodicals; Superréseaux -- Périodiques; Microstructure (Physique) -- Périodiques; Semiconducteurs -- Périodiques; 621.38152
• DOI: 10.1016/j.spmi.2017.04.041
• Languages: English
• ISSNs: 0749-6036

Abstract

Abstract: We report on ab-initio DFT/FP-LAPW/TB-mBJ/GGA and LDA investigation of structural and electronic properties of Mgx Zn1−x O alloys in Würtzite (WZ), Rocksalt (RS) and Zinc-Blende (ZB) phases. TB-mBJ corrections of electronic exchange and correlation interactions make it possible to improve considerably the computational results which we have found very close to the experimental data. As expected, our results show that at 0.375 < x < 0.5, Mgx Zn1−x O undergoes a phase transition from the tetrahedrally coordinated non-centrosymmetric covalent WZ phase to the octahedrally coordinated ionic RS phase, and the ZB phase remains metastable in the whole 0 ≤ x≤1 range. Our structural properties results show that the lattice parameters vary nonlinearly with x in all three phases. In ZB phase, aZB increases with x very slightly (ΔaZB /aZB ≤+0.6%) while in RS phase, aRS decreases with x more strongly (ΔaRS /aRS ≈ −1.7%). The strongest lattice parameters variations with x are found in WZ phase where increasing x results in increasing aWZ (ΔaWZ /aWZ ≈+1.4%), decreasing cWZ (ΔcWZ /cWZ ≈ −2.9%), decreasing cWZ /aWZ ratio (Δ(cWZ /aWZ )/(cWZ /aWZ )≈-3.31%), and increasing u internal parameter (Δu/u≈+2.8%). Our electronic properties results show that the fundamental energy bandgap EG is Γ-direct in WZ and ZB Mgx Zn1−x O in the whole 0 ≤ x≤1 range. In RS Mgx Zn1−x O, EG is indirect throughout 0 ≤ x < 1 range including RS ZnO and excluding RS MgO where EG is Γ-direct. In all three phases, EG increases with x first linearly in the low x range (x < 0.5), then nonlinearly at higher x (x≥0.5). At x < 0.5, EG ZB (x) = 2.609 + 2.861× eV, EG WZ (x) = 2.863 + 1.990× eV, and EG RS (x) = 3.190 + 1.508× eV. At x≥0.5, nonlinear EG (x) variations show strong bowing parameters depending on the crystal phase: bZB = 2.709eV, bWZ = 4.079eV, and bRS = 16.83eV. These strong EG (x) variations which are confined to a narrow high x range, are tightly correlated with the addition of Zn to MgO and are the strongest in RS Mgx Zn1−x O. Densities of states and energy band structure data analysis show dominant influence of strong exchange and correlation interactions between hybridized O:2p-Zn:3d orbitals which take place as soon as Zn is introduced into MgO. Our results confirm early findings that O:2p-Zn:3d interactions do play a leading role in overall Mgx Zn1−x O physical properties whatever the phase, with strongest effects in RS phase, especially in huge EG bowings and in RS-WZ phase transition. Highlights: DFT-FP-LAPW/TB-mBJ/LDA -GGA study of ZB, WZ, and RS Mgx Zn1−x O properties. Lattice parameters and energy bandgaps variations with x (0 ≤ x≤1). Evidence for hybridized O:2p-Zn:3d orbitals exchange and correlation interactions.