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多体微扰理论得到的精确表面和吸附能。

Accurate surface and adsorption energies from many-body perturbation theory.

出版信息

Nat Mater. 2010 Sep;9(9):741-4. doi: 10.1038/nmat2806. Epub 2010 Jul 25.

Abstract

Kohn-Sham density functional theory is the workhorse computational method in materials and surface science. Unfortunately, most semilocal density functionals predict surfaces to be more stable than they are experimentally. Naively, we would expect that consequently adsorption energies on surfaces are too small as well, but the contrary is often found: chemisorption energies are usually overestimated. Modifying the functional improves either the adsorption energy or the surface energy but always worsens the other aspect. This suggests that semilocal density functionals possess a fundamental flaw that is difficult to cure, and alternative methods are urgently needed. Here we show that a computationally fairly efficient many-electron approach, the random phase approximation to the correlation energy, resolves this dilemma and yields at the same time excellent lattice constants, surface energies and adsorption energies for carbon monoxide and benzene on transition-metal surfaces.

摘要

Kohn-Sham 密度泛函理论是材料和表面科学中常用的计算方法。不幸的是,大多数半局域密度泛函理论预测表面比实验更稳定。我们可能会认为,因此表面上的吸附能也太小了,但事实往往相反:化学吸附能通常被高估。修改泛函可以改善吸附能或表面能,但总是会恶化另一方面。这表明半局域密度泛函理论存在一个难以纠正的根本缺陷,因此迫切需要替代方法。在这里,我们展示了一种计算效率相当高的多电子方法,即关联能的随机相位近似,它解决了这一困境,同时为一氧化碳和苯在过渡金属表面上的晶格常数、表面能和吸附能提供了优异的结果。

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