First Principles Calculation of Al-Doped Mg/Mg2Sn Alloy Interface
WANG Furong1, ZHANG Yongmei1, BAI Guoning2, GUO Qingwei2, ZHAO Yuhong2,3()
1School of Semiconductors and Physics, North University of China, Taiyuan 030051, China 2School of Materials Science and Engineering, North University of China, Taiyuan 030051, China 3Beijing Advanced Innovation Center for Materials Genome Engineering, University of Science and Technology Beijing, Beijing 100083, China
Cite this article:
WANG Furong, ZHANG Yongmei, BAI Guoning, GUO Qingwei, ZHAO Yuhong. First Principles Calculation of Al-Doped Mg/Mg2Sn Alloy Interface. Acta Metall Sin, 2023, 59(6): 812-820.
Mg-Sn alloy is a high temperature-creep resistant magnesium alloy that has potential applications in lightweight automobiles. The addition of Sn to Mg can reduce the overall cost of the alloy as Sn is cheaper than rare earth elements. Sn and Mg form Mg2Sn phase on the grain boundary, and this Mg2Sn phase has an excellent precipitation hardening effect. However, coarsened Mg2Sn phase can reduce the age hardening effect of the alloy. Previous experimental studies have showed that the addition of Al element can considerably improve the age hardening effect of Mg-Sn alloy as it segregated at the interface between the Mg matrix and Mg2Sn phase. However, there is a lack of research on the different orientations of Al-doped Mg matrix and Mg2Sn phase and the distribution position of Al element at the interface. Therefore, in this study, the interface adhesion energy, interface energy, and interface doping energy of Al-doped Mg/Mg2Sn with different index surfaces were calculated based on density functional theory to determine more stable doping positions. The effects of Al doping on the electronic structure of Mg(0001)/Mg2Sn(022) interface were analyzed using the density of states and crystal orbital Hamilton population. The results demonstrate that only a part of the Al-doping positions is beneficial in strengthening the stability of Mg/Mg2Sn interface. After the addition of Al, the adhesion energy of Sn termination at Mg(0001)/Mg2Sn(001) interface is higher than that of Mg termination, but the adhesion energy of Sn termination at Mg(0001)/Mg2Sn(111) interface is lower than that of Mg termination. In addition, the interface energy of Mg(0001)/Mg2Sn(022) interface doped with Al decreased by 0.07 eV/nm compared to that of Mg(0001)/Mg2Sn(022) interface. The addition of Al element to Mg(0001)/Mg2Sn(022) facilitates the doping of a special position, which shows an obvious interaction between the s orbital of Al and the p orbital of Sn after Al doping. Moreover, the Al—Sn bonding is found to be dominant at the interface.
Fund: National Natural Science Foundation of China(52074246);National Natural Science Foundation of China(22008224);National Natural Science Foundation of China(52275390);National Natural Science Foundation of China(52205429);National Natural Science Foundation of China(52201146);National Defense Basic Scientific Research Program of China(JCKY20204-08B002);National Defense Basic Scientific Research Program of China(WDZC2022-12);Key Research and Development Program of Shanxi Province(202102050-201011);Guiding Local Science and Technology Development Projects by the Central Government(YDZJSX-2022A025);Guiding Local Science and Technology Development Projects by the Central Government(YDZJSX2021A027)
Corresponding Authors:
ZHAO Yuhong, professor, Tel:15035172958, E-mail: zhaoyuhong@nuc.edu.cn
Table 1 Interface spacing, interface energy, and lattice mismatch degree of Mg/Mg2Sn
Fig.1 Schematics of Mg/Mg2Sn interface model with different interface orientations doped with Al element (Roman numerals represent the different doping positions of Al at the interface) (a, b) Mg terminal (a) and Sn terminal (b) models of Mg(0001)/Mg2Sn(001) interface, respectively (c) Mg(0001)/Mg2Sn(022) interface model (d, e) Mg terminal (d) and Sn terminal (e) models of Mg(0001)/Mg2Sn(111) interface, respectively
Fig.2 Adhesion energies of Mg/Mg2Sn interface with doping Al element at different positions (Dotted lines represent the interface adhesion energies without Al element)
Position
Interface spacing / nm
Interface energy / (J·m-2)
Interface doping energy / (J·m-2)
Ⅰ
25.84
0.418
-5.031
Ⅱ
23.64
0.143
-5.070
Ⅲ
23.20
0.140
-5.076
Ⅳ
22.83
0.091
-5.079
Ⅴ
23.22
0.149
-5.075
Ⅵ
23.27
0.152
-5.075
Table 2 Interface spacing, interface energy, and doping energy of Al-doped Mg(0001)/Mg2Sn(022) interface
Fig.3 Interface energies of Mg(0001)/Mg2Sn(022) before (a) and after (b) doping Al element at position IV in Fig.1c (The intercept of the line in the figure represents the elastic strain energy, and the slope represents the interface energy. A—interface area, N—number of atoms in the interface, ΔGf—energy contained in a single atom in the interface)
Fig.4 Partial density of states (PDOS) curves of Mg(0001)/Mg2Sn(022) interface before (a) and after (b) doping Al element at position IV in Fig.1c (EF—Fermi level)
Fig.5 Side views (a1, b1) and top views (a2, b2) of differential charge density diagrams of the Mg(0001)/Mg2Sn(022) interface before (a1, a2) and after (b1, b2) doping Al element at position IV in Fig.1c (The red areas represent the accumulation of electric charge, and the blue areas represent the loss of electric charge)
Fig.6 Projected crystal orbital Hamilton population (pCOHP) curves of hcp Mg (a) and fcc Mg2Sn (b); Mg—Mg (c) and Mg—Sn (d) atoms at the Mg(0001)/Mg2Sn(022) interface; and Mg—Al (e) and Al—Sn (f) atoms at the Mg(0001)/Mg2Sn(022) interface after doping Al (ICOHP—integrated crystal orbital Hamilton population)
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