摘要
The structural, elastic, phonon and electronic properties of a MnPd alloy have been investigated using the first- principles calculation. The calculated lattice constants and electronic structure agree well with the experimental results. The microscopic mechanism of the diffusionless martensitic transition from the paramagnetic B2 （PM-B2） phase to the antiferromagnetic L10 （AFM-L10） phase through the intermediate paramagnetic L10 （PM-L10） phase has been explored theoretically. The obtained negative shear modulus C＇ - （C11 - C12）/2 of the PM-B2 phase is closely related to the instability of the cubic B2 phase with respect to the tetragonal distortions. The calculated phonon dispersions for the PM-L10 and AFM-L10 phases indicate that they are dynamically stable. However, the AFM-L10 phase is energetically most favorable according to the calculated total energy order, so the PM-L10 -＋AFM-L10 transition is caused by the magnetism rather than the electron-phonon interaction. Additionally, the AFM-L10 state is stabilized through the formation of a pseudo gap located at the Fermi level. The calculated results show that the CuAu-I type structure in the collinear antiferromagnetic state is dynamically and mechanically stable, thus is the low temperature phase.
The structural, elastic, phonon and electronic properties of a MnPd alloy have been investigated using the first- principles calculation. The calculated lattice constants and electronic structure agree well with the experimental results. The microscopic mechanism of the diffusionless martensitic transition from the paramagnetic B2 （PM-B2） phase to the antiferromagnetic L10 （AFM-L10） phase through the intermediate paramagnetic L10 （PM-L10） phase has been explored theoretically. The obtained negative shear modulus C＇ - （C11 - C12）/2 of the PM-B2 phase is closely related to the instability of the cubic B2 phase with respect to the tetragonal distortions. The calculated phonon dispersions for the PM-L10 and AFM-L10 phases indicate that they are dynamically stable. However, the AFM-L10 phase is energetically most favorable according to the calculated total energy order, so the PM-L10 -＋AFM-L10 transition is caused by the magnetism rather than the electron-phonon interaction. Additionally, the AFM-L10 state is stabilized through the formation of a pseudo gap located at the Fermi level. The calculated results show that the CuAu-I type structure in the collinear antiferromagnetic state is dynamically and mechanically stable, thus is the low temperature phase.
基金
Project supported by the National Natural Science Foundation of China (Grant Nos. 10647008 and 50971099)
the Research Fund for the Doctoral Program of Higher Education, China (Grant No. 20096101110017)
