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来自非共线自旋密度泛函微扰理论的磁交换耦合

Magnetic exchange couplings from noncollinear spin density functional perturbation theory.

作者信息

Peralta Juan E, Barone Veronica

机构信息

Department of Physics, Central Michigan University, Mt. Pleasant, Michigan 48859, USA.

出版信息

J Chem Phys. 2008 Nov 21;129(19):194107. doi: 10.1063/1.3013602.

Abstract

We propose a method for the evaluation of magnetic exchange couplings based on noncollinear spin density functional calculations. The method employs the second derivative of the total Kohn-Sham energy of a single reference state, in contrast to approximations based on Kohn-Sham total energy differences. The advantage of our approach is twofold: It provides a physically motivated picture of the transition from a low-spin to a high-spin state, and it utilizes a perturbation scheme for the evaluation of magnetic exchange couplings. The latter simplifies the way these parameters are predicted using first principles: It avoids the nontrivial search for different spin states that needs to be carried out in energy difference methods, and it opens the possibility of "black-boxifying" the extraction of exchange couplings from density functional theory calculations. We present proof of concept calculations of magnetic exchange couplings in the H-He-H model system and in an oxovanadium bimetallic complex where the results can be intuitively rationalized.

摘要

我们提出了一种基于非共线自旋密度泛函计算来评估磁交换耦合的方法。与基于Kohn-Sham总能差的近似方法不同,该方法采用单个参考态的总Kohn-Sham能量的二阶导数。我们方法的优点有两个方面:它提供了从低自旋态到高自旋态转变的物理动机图像,并且它利用微扰方案来评估磁交换耦合。后者简化了使用第一性原理预测这些参数的方式:它避免了在能量差方法中对不同自旋态进行的复杂搜索,并且开启了从密度泛函理论计算中“黑箱化”提取交换耦合的可能性。我们给出了H-He-H模型系统和一个氧钒双金属配合物中磁交换耦合的概念验证计算,其中结果可以直观地合理化。

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