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一种无自相互作用的局域杂化泛函:相对于来自科恩-沈本征值的精确电离势而言的精确结合能。

A self-interaction-free local hybrid functional: accurate binding energies vis-à-vis accurate ionization potentials from Kohn-Sham eigenvalues.

作者信息

Schmidt Tobias, Kraisler Eli, Makmal Adi, Kronik Leeor, Kümmel Stephan

机构信息

Theoretical Physics IV, University of Bayreuth, 95440 Bayreuth, Germany.

Department of Materials and Interfaces, Weizmann Institute of Science, Rehovoth 76100, Israel.

出版信息

J Chem Phys. 2014 May 14;140(18):18A510. doi: 10.1063/1.4865942.

Abstract

We present and test a new approximation for the exchange-correlation (xc) energy of Kohn-Sham density functional theory. It combines exact exchange with a compatible non-local correlation functional. The functional is by construction free of one-electron self-interaction, respects constraints derived from uniform coordinate scaling, and has the correct asymptotic behavior of the xc energy density. It contains one parameter that is not determined ab initio. We investigate whether it is possible to construct a functional that yields accurate binding energies and affords other advantages, specifically Kohn-Sham eigenvalues that reliably reflect ionization potentials. Tests for a set of atoms and small molecules show that within our local-hybrid form accurate binding energies can be achieved by proper optimization of the free parameter in our functional, along with an improvement in dissociation energy curves and in Kohn-Sham eigenvalues. However, the correspondence of the latter to experimental ionization potentials is not yet satisfactory, and if we choose to optimize their prediction, a rather different value of the functional's parameter is obtained. We put this finding in a larger context by discussing similar observations for other functionals and possible directions for further functional development that our findings suggest.

摘要

我们提出并测试了一种用于科恩-沙姆密度泛函理论交换关联(xc)能量的新近似方法。它将精确交换与一种兼容的非局部关联泛函相结合。该泛函在构建时无单电子自相互作用,满足从均匀坐标缩放导出的约束条件,并且具有xc能量密度的正确渐近行为。它包含一个非从头算确定的参数。我们研究是否有可能构建一种能给出精确结合能并具有其他优势的泛函,特别是能可靠反映电离势的科恩-沙姆本征值。对一组原子和小分子的测试表明,在我们的局域杂化形式中,通过适当优化泛函中的自由参数,以及改进解离能曲线和科恩-沙姆本征值,可以实现精确的结合能。然而,后者与实验电离势的对应关系仍不令人满意,并且如果我们选择优化它们的预测,会得到泛函参数的一个相当不同的值。我们通过讨论其他泛函的类似观察结果以及我们的发现所暗示的进一步泛函发展的可能方向,将这一发现置于更广泛的背景中。

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