机构地区:[1]School of Communication and Electronic Engineering, Hunan City University [2]School of Physics and Electronics,Central South University
出 处:《Journal of Wuhan University of Technology(Materials Science)》2018年第3期566-570,共5页武汉理工大学学报(材料科学英文版)
基 金:Funded by the National Natural Science Foundation of China(Nos.11547186,11604091);the Natural Science Foundation of Hunan Province(No.2018JJ2019);the Research Foundation of Education Bureau of Hunan Province,China(No.16B048)
摘 要:The spontaneous magnetic transitions and corresponding magnetoelastic properties of intermetallic compounds RMn2Ge2(R=Gd, Tb and Dy) were investigated by using the X-ray diffraction method and magnetic measurement. The results showed that the compounds experience two magnetic transitions, namely the second-order paramagnetic to antiferromagnetic transition at temperature TN(TN=368, 423 and 443 K for Gd Mn2 Ge2, Tb Mn2 Ge2 and Dy Mn2 Ge2, respectively) and the first-order antiferromagnetic-ferrimagnetic transition at temperature Tt(Tt=96, 80 and 40 K for Gd Mn2 Ge2, Tb Mn2 Ge2 and Dy Mn2 Ge2, respectively) as the temperature decreases. The temperature dependence of the lattice constant a(T) displays a negative magnetoelastic anomaly at the second-order transition point TN and, at the first-order transition Tt, a increases abruptly for Gd Mn2 Ge2 and Tb Mn2 Ge2, Da/a about 10^(-3). Nevertheless, the lattice constant c almost does not change at these transition points indicating that such magnetoelastic anomalies are mainly contributed by the Mn-sublattice. The transitions of the magnetoelastic properties are also evidenced on the temperature dependence of magnetic susceptibility χ. The first-order transition behavior at Tt is explained by the Kittel mode of exchange inversion.The spontaneous magnetic transitions and corresponding magnetoelastic properties of intermetallic compounds RMn2Ge2(R=Gd, Tb and Dy) were investigated by using the X-ray diffraction method and magnetic measurement. The results showed that the compounds experience two magnetic transitions, namely the second-order paramagnetic to antiferromagnetic transition at temperature TN(TN=368, 423 and 443 K for Gd Mn2 Ge2, Tb Mn2 Ge2 and Dy Mn2 Ge2, respectively) and the first-order antiferromagnetic-ferrimagnetic transition at temperature Tt(Tt=96, 80 and 40 K for Gd Mn2 Ge2, Tb Mn2 Ge2 and Dy Mn2 Ge2, respectively) as the temperature decreases. The temperature dependence of the lattice constant a(T) displays a negative magnetoelastic anomaly at the second-order transition point TN and, at the first-order transition Tt, a increases abruptly for Gd Mn2 Ge2 and Tb Mn2 Ge2, Da/a about 10^(-3). Nevertheless, the lattice constant c almost does not change at these transition points indicating that such magnetoelastic anomalies are mainly contributed by the Mn-sublattice. The transitions of the magnetoelastic properties are also evidenced on the temperature dependence of magnetic susceptibility χ. The first-order transition behavior at Tt is explained by the Kittel mode of exchange inversion.
关 键 词:rare earth-transition metal compound magnetic transition magnetoelastic property
分 类 号:TM271[一般工业技术—材料科学与工程]
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