First-principle studies on the mechanical, thermodynamic and electronic properties of β″-Mg3Gd and β′-Mg7Gd alloys under pressure. (February 2019)

• Record Type: Journal Article
• Authors: Wang, Shuo; Zhao, Yuhong; Deng, Shijie; Yang, Wenkui; Lian, Dongxiao; Hou, Hua
• Is Part Of: Journal of physics and chemistry of solids. Volume 125(2019)
• Page Start: 115
• Page End: 122
• Publication Date: 2019-02
• Subjects: Precipitates -- Mechanical properties -- Electronic properties -- Thermodynamic properties; Solids -- Periodicals; Solides -- Périodiques; Solids; Periodicals; 530.41
• DOI: 10.1016/j.jpcs.2018.10.020
• Languages: English
• ISSNs: 0022-3697

Abstract

Abstract: A theoretical investigation on the mechanical, thermodynamic and electronic properties of β″-Mg3 Gd and β′-Mg7 Gd compounds at the effect of pressure have been conducted through the first-principles calculations. Since the shear modulus of β″ is less affected by pressure, its bulk modulus/shear modulus ( B / G ) is more sensitive to pressure than β′. Based on the analysis of vibrational heat capacity C V, β′ can absorb more heat at high temperature. The pressure-induced distribution of charges is more localized between atoms, making stronger covalent bonds. Further, the inhomogeneous distributions of covalent and metal bonds may be the reason for the increased anisotropy based on the Ranganathan's anisotropy index ( A U ). The Mg p and the Gd d states expand to both occupied and unoccupied states, whereas the lower energy Mg s and Gd s, p states expand primarily to bonding states under high pressures. The spatial distributions of Mg p and Gd d electrons hybridization at antibonding states act a crucial role in improving mechanical properties of alloys at the applied pressure. Graphical abstract: Highlights: The B/G of β″-Mg3 Gd becomes larger than β′-Mg7 Gd with increasing pressure because of less growing shear modulus. The electron localization function reveals the cause of the increasing anisotropic. Different spatial distributions of Mg p and Gd d electrons hybridize at antibonding states.