Temperature dependence of elastic properties of Ni2+xMn1xGa and Ni2Mn(Ga1xAlx) from first principles

Chun-Mei Li, Hu-Bin Luo, Qing-Miao Hu, Rui Yang, Börje Johansson, and Levente Vitos
Phys. Rev. B 84, 174117 – Published 22 November 2011

Abstract

The temperature dependence of the elastic properties of Ni2+xMn1xGa and Ni2Mn(Ga1xAlx) (x=0.0, 0.1, and 0.2) random alloys are investigated by using the first-principles exact muffin-tin orbitals method. At 0 K, the calculated equilibrium parameters in both cubic L21 and nonmodulated tetragonal β-Ni2MnGa are in good agreement with the available experimental data and other theoretical results. Separating the thermal effects into single electron excitation, volume expansion, phonon smearing, and magnetic terms, we find that phonon smearing gives the dominating positive tetragonal elastic constant (C) versus temperature (T) slope for the cubic phase. For Ni2+xMn1xGa, the competition between the negative alloying effect (C/x<0) and the positive temperature effect (C/T>0) leads to nearly constant C[x,TM(x)] at the martensitic transition temperature TM(x). For Ni2Mn(Ga1xAlx), where both C/x and C/T are positive, however, due to the significantly decrease of TM(x), the critical C[x,TM(x)] slightly decreases with Al doping. Furthermore, it is demonstrated that both the composition and the temperature dependence of C are indispensable to get a reasonable theoretical TM(x).

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  • Received 22 August 2011

DOI:https://doi.org/10.1103/PhysRevB.84.174117

©2011 American Physical Society

Authors & Affiliations

Chun-Mei Li1,2, Hu-Bin Luo2, Qing-Miao Hu2,*, Rui Yang2, Börje Johansson1,3,4, and Levente Vitos1,3,5

  • 1Applied Materials Physics, Department of Materials Science and Engineering, Royal Institute of Technology, Stockholm SE-100 44, Sweden
  • 2Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, 72 Wenhua Road, Shenyang 110016, China
  • 3Condensed Matter Theory Group, Physics Department, Uppsala University, P. O. Box 516, SE-75120 Uppsala, Sweden
  • 4School of Physics and Optoelectronic Technology & College of Advanced Science and Technology Dalian University of Technology, Dalian 116024, China
  • 5Research Institute for Solid State Physics and Optics, Budapest H-1525, P. O. Box 49, Hungary

  • *qmhu@imr.ac.cn

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Vol. 84, Iss. 17 — 1 November 2011

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