首页> 外文期刊>MATEC Web of Conferences >Accuracy of Real Space Cluster Expansion for Total Energies of Pd-rich PdX (X=Rh, Ru) Alloys, based on Full-Potential KKR Calculations for Perfect and Impurity Systems
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Accuracy of Real Space Cluster Expansion for Total Energies of Pd-rich PdX (X=Rh, Ru) Alloys, based on Full-Potential KKR Calculations for Perfect and Impurity Systems

机译:基于完善和杂质系统的全势KKR计算,富PdX(X = Rh,Ru)合金的总能量的实空间簇扩展精度

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We study the accuracy and convergence of the real space cluster expansion (RSCE) for the total energies of the Pd-rich PdX (X=Ru, Rh) alloys, which are used to study the phase stability and phase equilibria of the Pd-rich PdX alloys. In the present RSCE, the X atoms of minor element are treated as impurities in Pd. The n -body interaction energies (IEs) among X impurities in Pd, being used in the expansion of the total energies of the Pd-rich PdX alloys, are determined uniquely and successively from the low body to high body, by the full-potential Korringa-Kohn-Rostoker (FPKKR) Green's function method (FPKKR) for the perfect and impurity systems (Pd-host and X_( n )in Pd, n =1~4), combined with the generalized gradient approximation in the density functional theory. In the previous paper, we showed that the RSCE, in which the perturbed potentials due to the insertion of X_( n )impurities in Pd were redetermined self-consistently up to the first-nearest neighboring ( nn ) host atoms around X_( n )impurities, reproduce fairly well (the error of ~ 0.2mRy per atom) the FPKKR-band-calculation result of the ordered Pd_(3)Rh alloy in L1_(2)structure, but a little wrongly (the error of ~ 0.7mRy per atom) for the ordered Pd_(3)Ru alloy in L1_(2)structure. In the present paper, we show that this small RSCE error for the Pd3Ru alloy is corrected very well (from ~ 0.7mRy to ~ 0.1mRy per atom) by enlarging the self-consistent region for the perturbed potentials up to the 2nd-nn host atoms around Run impurities in Pd. We also clarify the correction for each value of the n-body ( n =1~ 4) IEs.
机译:我们研究了富含Pd的PdX(X = Ru,Rh)合金的总能量的实空间簇扩展(RSCE)的准确性和收敛性,用于研究富含Pd的相稳定性和相平衡PdX合金。在当前的RSCE中,微量元素的X原子被视为Pd中的杂质。 Pd中X杂质之间的n体相互作用能(IEs)用于富Pd PdX合金总能量的扩展,由全势从低体到高体唯一地依次确定Korringa-Kohn-Rostoker(FPKKR)格林函数方法(FPKKR)用于完美和杂质系统(Pd-host和Pd中的X_(n),n = 1〜4),并结合了密度泛函理论中的广义梯度近似。在先前的论文中,我们显示了RSCE,其中自一致地重新确定了Pd中X_(n)杂质插入引起的扰动电势,直到X_(n)附近的第一个最近邻(nn)个宿主原子为止。杂质,在L1_(2)结构中有序Pd_(3)Rh合金的FPKKR能带计算结果重现相当好(每个原子的误差约为0.2mRy),但有一点不对(每个原子的误差约为0.7mRy) L1_(2)结构的有序Pd_(3)Ru合金)。在本文中,我们表明,通过将扰动电势的自洽区域扩大到2 nn主体,可以很好地校正Pd3Ru合金的这种较小RSCE误差(从每个原子〜0.7mRy到〜0.1mRy)。 Pd中的杂质周围的原子。我们还阐明了对n体(n = 1〜4)个IE的每个值的校正。

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