Band structure, density of states, and crystal chemistry of ZrGa2 and ZrGa3 single crystals

• Published in: Journal of alloys and compounds 2013-04, Vol.556, p.259-265
• Main Authors: Reshak, A.H., Lakshminarayana, G., Ebothe, J., Fedorchuk, A.O., Fedyna, M.F., Kamarudin, H., Mandracci, P., Auluck, S.
• Format: Article
• Language: English
• Subjects: A. Inorganic materials; Alloys; B. Crystal growth; Band structure of solids; C. Electronic band structure; Charge density; Chemical bonds; Condensed matter: electronic structure, electrical, magnetic, and optical properties; Condensed matter: structure, mechanical and thermal properties; Crystal structure; D. X-ray diffraction; Density of states; Dispersions; Electron density of states and band structure of crystalline solids; Electron states; Exact sciences and technology; Mathematical analysis; Physics; Structure of solids and liquids; crystallography; Structure of specific crystalline solids; Unit cell
• ISSN: 0925-8388; 1873-4669
• DOI: 10.1016/j.jallcom.2012.12.138

[Display omitted] ► ZrGa2 and ZrGa3 crystals structure was analyzed. ► FP-LAPW method was used to solve the Kohn Sham DFT equations within the framework of the WIEN2K code. ► Electronic band structures are reported. ► The studied crystals exhibit potential optoelectronic applications. Using FP-LAPW Method we have performed calculations of the band structure of the ZrGa2 and ZrGa3 crystals. The all-electron full potential linearized augmented plane wave method was used to solve the Kohn Sham DFT equations. We have explored different approximations using three kinds of exchange-correlation potentials on the electronic structure and we concluded that there is insignificant influence on the band structure and the density of states. It is clear that there exists a difference in the band dispersion with one move from ZrGa2 to ZrGa3 that is attributed to the fact that ZrGa2 has four formula per unit cell (Z=4) while ZrGa3 has two formula per unit cell (Z=2). Despite some similarity in the crystallochemistry of ZrGa2 to ZrGa3 some differences are observed in the band structure dispersion. There is a strong hybridization between the states. The interaction of charges between Zr and Ga atoms is due to the strong hybridization, and the covalent bond arises due to the degree of hybridization. Hence, there is a strong covalent bonding between these atoms. We have obtained a space electron charge density distribution in the average unit cell by calculations of the electron charge density distribution. The space electronic charge density contour distribution is illustrated in (100) and (110) planes.