TY - JOUR
T1 - Effects of Ni substitution on magnetism and thermal expansion of antiperovskite Mn3Ga1-xNixN (0 ≤ x ≤ 1.0)
AU - Lu, Huiqing
AU - Sun, Ying
AU - Shi, Kewen
AU - Wang, Lei
AU - Wang, Wei
AU - Huang, Rongjing
AU - Yuan, Xiuliang
AU - Yan, Jun
AU - Diao, Xungang
AU - Wang, Cong
N1 - Publisher Copyright:
© 2018 Elsevier Ltd and Techna Group S.r.l.
PY - 2018/6/1
Y1 - 2018/6/1
N2 - Effects of Ni substitution on magnetic and thermal expansion properties in Mn3Ga1−xNixN (0 ≤ x ≤ 1.0) were investigated. The magnetic structure for Mn3GaN is a typical noncollinear antiferromagnetic Γ5 g. After Ni was introduced to the Ga site, the spin alignment was changed from antiferromagnetic to ferromagnetic. In addition, the magnetic transition temperature first decreased and then increased with increasing Ni content, which could be ascribed to the competition between the electron-type doping effect and the lattice effect. Near the magnetic transition, Mn3Ga1−xNixN showed an abrupt lattice contraction with increasing temperature and the magnitude of the lattice contraction gradually decreased from 0.38% (for x = 0) to 0.09% (for x = 1.0) with increasing Ni substitution. In particular, zero thermal expansion behavior below 150 K was observed in Mn3Ga.6Ni.4N, and thermal expansion coefficient α was estimated to be 0.311 × 10−6 K−1. The obtained zero thermal expansion is very useful for practical applications in precision devices. The zero thermal expansion behavior was assumed to be associated with the ferromagnetic characteristic induced by the Ni substitution, which stabilized the Γ5 g antiferromagnetic structure.
AB - Effects of Ni substitution on magnetic and thermal expansion properties in Mn3Ga1−xNixN (0 ≤ x ≤ 1.0) were investigated. The magnetic structure for Mn3GaN is a typical noncollinear antiferromagnetic Γ5 g. After Ni was introduced to the Ga site, the spin alignment was changed from antiferromagnetic to ferromagnetic. In addition, the magnetic transition temperature first decreased and then increased with increasing Ni content, which could be ascribed to the competition between the electron-type doping effect and the lattice effect. Near the magnetic transition, Mn3Ga1−xNixN showed an abrupt lattice contraction with increasing temperature and the magnitude of the lattice contraction gradually decreased from 0.38% (for x = 0) to 0.09% (for x = 1.0) with increasing Ni substitution. In particular, zero thermal expansion behavior below 150 K was observed in Mn3Ga.6Ni.4N, and thermal expansion coefficient α was estimated to be 0.311 × 10−6 K−1. The obtained zero thermal expansion is very useful for practical applications in precision devices. The zero thermal expansion behavior was assumed to be associated with the ferromagnetic characteristic induced by the Ni substitution, which stabilized the Γ5 g antiferromagnetic structure.
KW - Antiperovskite manganese nitride
KW - Magnetic transition
KW - Zero thermal expansion
UR - https://www.scopus.com/pages/publications/85042914333
U2 - 10.1016/j.ceramint.2018.02.180
DO - 10.1016/j.ceramint.2018.02.180
M3 - 文章
AN - SCOPUS:85042914333
SN - 0272-8842
VL - 44
SP - 9574
EP - 9580
JO - Ceramics International
JF - Ceramics International
IS - 8
ER -