Abstract:
The martensitic transformation, mechanical, and magnetic properties of the Ni
2Mn
1.5−xCu
xTi
0.5 (
x = 0.125, 0.25, 0.375, 0.5) and Ni
2−yCo
yMn
1.5−xCu
xTi
0.5 (
x = 0.125,
y = 0.125, 0.25, 0.375, 0.5) and (
x = 0.125, 0.25, 0.375,
y = 0.625) alloys were systematically studied by the first-principles calculations. For the formation energy, the martensite is smaller than the austenite, the Ni–(Co)–Mn–Cu–Ti alloys studied in this work can undergo martensitic transformation. The austenite and non-modulated (NM) martensite always present antiferromagnetic state in the Ni
2Mn
1.5−xCu
xTi
0.5 and Ni
2−yCo
yMn
1.5−xCu
xTi
0.5 (
y < 0.625) alloys. When
y = 0.625 in the Ni
2−yCo
yMn
1.5−xCu
xTi
0.5 series, the austenite presents ferromagnetic state while the NM martensite shows antiferromagnetic state. Cu doping can decrease the thermal hysteresis and anisotropy of the Ni–(Co)–Mn–Ti alloy. Increasing Mn and decreasing Ti content can improve the shear resistance and normal stress resistance, but reduce the toughness in the Ni–Mn–Cu–Ti alloy. And the ductility of the Co–Cu co-doping alloy is inferior to that of the Ni–Mn–Cu–Ti and Ni–Co–Mn–Ti alloys. The electronic density of states was studied to reveal the essence of the mechanical and magnetic properties.