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Anomalous thermodynamic properties and phase stability of δ-Pu_(1-x)M_x (M=Ga and Al)alloys from first-principles calculations

机译:从第一性原理计算得出δ-Pu_(1-x)M_x(M = Ga和Al)合金的异常热力学性质和相稳定性

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摘要

The composition-dependent crystal structure, volume, elastic constants, and electronic structure of δ-Pu_(1-x)M_x (M = Ga and Al, 0 ≤ x ≤ 0.1) alloys are systematically studied by using first-principles EMTO-CPA calculations. It is shown that the fcc and Ll_2 structures co-exist in the alloys with x ≤ 0.04 whereas for x > 0.04, the L1_2 structure is more and more preferable and around x = 0.1, it tends to be stabilized alone. The evaluated V ~ x of the Ll_2 structure, being negative deviation from Vegard's law, turns out to be in good agreement with the experimental result. For x ≤ 0.04, the estimated E, G, v, and Θ of both the fcc and L1_2 structures are in line with the measured data, whereas when x > 0.04, only those of the L1_2 structure are close to the experimental results. The electronic hybridization between Pu and M atoms is dominated by Pu for the s, d, and f states but M for the p state. The strong interactions between Pu and M atoms in the same site of the L1_2 structure should be responsible for its relative stability in the alloys with x > 0.04. The electron-phonon coupling further decreases the phase stability of δ-Pu_(1-x)M_x with increasing x.
机译:使用第一性原理EMTO-CPA系统研究了δ-Pu_(1-x)M_x(M = Ga和Al,0≤x≤0.1)合金的成分依赖性晶体结构,体积,弹性常数和电子结构计算。结果表明,在x≤0.04的合金中,fcc和Ll_2结构共存,而对于x> 0.04,则越来越优选L1_2结构,并且在x = 0.1附近,倾向于单独稳定化。与Vegard定律的负偏差表明,Ll_2结构的V〜x值与实验结果吻合良好。对于x≤0.04,fcc和L1_2结构的估计E,G,v和Θ与测量数据一致,而当x> 0.04时,只有L1_2结构的E,G,v和Θ与实验结果接近。 Pu和M原子之间的电子杂化主要由Pu代表s,d和f状态,而M代表p状态。在x> 0.04的合金中,P1和M原子在L1_2结构的相同位置之间的强相互作用应负责其相对稳定性。电子声子耦合随着x的增加进一步降低了δ-Pu_(1-x)M_x的相位稳定性。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2016年第21期|214108.1-214108.8|共8页
  • 作者单位

    College of Physical Science and Technology, Shenyang Normal University, Shenyang 110034, China,Shenyang National Laboratory for Materials Science, Institute of Metal Research,Chinese Academy of Sciences, 72 Wenhua Road, Shenyang 110016, China;

    Shenyang National Laboratory for Materials Science, Institute of Metal Research,Chinese Academy of Sciences, 72 Wenhua Road, Shenyang 110016, China;

    Applied Materials Physics, Department of Materials Science and Engineering, Royal Institute of Technology, Stockholm SE-100 44, Sweden,Condensed Matter Theory Group, Physics Department, Uppsala University, P.O. Box 516, SE-75120 Uppsala, Sweden,School of Physics and Optoelectronic Technology & College of Advanced Science and Technology Dalian University of Technology, Dalian 116024, China;

    Applied Materials Physics, Department of Materials Science and Engineering, Royal Institute of Technology, Stockholm SE-100 44, Sweden,Condensed Matter Theory Group, Physics Department, Uppsala University, P.O. Box 516, SE-75120 Uppsala, Sweden,Research Institute for Solid State Physics and Optics, Budapest H-1525, P.O. Box 49, Hungary;

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