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重新审视用于生物模拟的科恩-沈密度泛函的伪像。

Revisiting Artifacts of Kohn-Sham Density Functionals for Biosimulation.

作者信息

Slattery Samuel A, Yon Jaden C, Valeev Edward F

机构信息

Department of Chemistry, Virginia Tech, Blacksburg, Virginia 24061, United States.

出版信息

J Chem Theory Comput. 2024 Aug 13;20(15):6652-6660. doi: 10.1021/acs.jctc.4c00712. Epub 2024 Jul 31.

DOI:10.1021/acs.jctc.4c00712
PMID:39083031
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11325537/
Abstract

We revisit the problem of unphysical charge density delocalization/fractionalization induced by the self-interaction error of common approximate Kohn-Sham (KS) density functional theory functionals on simulation of small to medium-sized proteins in a vacuum. Aside from producing unphysical electron densities and total energies, the vanishing of the HOMO-LUMO gap associated with the unphysical charge delocalization leads to an unphysical low-energy spectrum and catastrophic failure of most popular solvers for the KS self-consistent field (SCF) problem. We apply a robust quasi-Newton SCF solver [ 2024, 26, 6557] to obtain solutions for some of these difficult cases. The anatomy of the charge delocalization is revealed by the obtained from the density matrix difference between the Hartree-Fock and KS solutions; the charge delocalization not only can occur between charged fragments (such as in zwitterionic polypeptides) but also involves neutral fragments. The vanishing-gap phenomenon and troublesome SCF convergence are both attributed to the unphysical KS Fock operator eigenspectra of molecular fragments (e.g., amino acids or their side chains). Analysis of amino acid pairs suggests that the unphysical charge delocalization can be partially ameliorated by the use of range-separated hybrid functionals but not by semilocal or standard hybrid functionals. Last, we demonstrate that solutions without the unphysical charge delocalization can be located even for semilocal KS functionals highly prone to such defects, but such solutions have non-Aufbau character and are unstable with respect to mixing of the non-overlapping "frontier" orbitals. Caution should be exercised when unexpectedly small (or vanishing) HOMO-LUMO gaps and atypical SCF convergence patterns (e.g., oscillatory) are observed in KS DFT simulations in any context (bio or otherwise).

摘要

我们重新审视了常见的近似Kohn-Sham(KS)密度泛函理论泛函的自相互作用误差在真空中模拟中小尺寸蛋白质时所引起的非物理电荷密度离域/分数化问题。除了产生非物理电子密度和总能量外,与非物理电荷离域相关的最高占据分子轨道(HOMO)-最低未占据分子轨道(LUMO)能隙的消失导致了非物理的低能谱以及大多数流行的KS自洽场(SCF)问题求解器的灾难性失败。我们应用一种稳健的拟牛顿SCF求解器[2024, 26, 6557]来获得其中一些难题的解决方案。通过从Hartree-Fock和KS解之间的密度矩阵差得到的结果揭示了电荷离域的剖析;电荷离域不仅可以发生在带电片段之间(如两性离子多肽中),还涉及中性片段。能隙消失现象和麻烦的SCF收敛都归因于分子片段(如氨基酸或其侧链)的非物理KS福克算子本征谱。氨基酸对的分析表明,使用范围分离的杂化泛函可以部分改善非物理电荷离域,但半局域或标准杂化泛函则不行。最后,我们证明即使对于极易出现此类缺陷的半局域KS泛函,也可以找到没有非物理电荷离域的解,但这些解具有非构造特征,并且相对于非重叠“前沿”轨道的混合是不稳定的。在任何情况下(生物或其他情况)的KS DFT模拟中,当观察到意外小(或消失)的HOMO-LUMO能隙和非典型的SCF收敛模式(如振荡)时,都应谨慎行事。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/86864985b97b/ct4c00712_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/3daf333e4965/ct4c00712_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/ec9f536d1e6e/ct4c00712_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/db619b75c029/ct4c00712_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/5b31c176e968/ct4c00712_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/86864985b97b/ct4c00712_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/3daf333e4965/ct4c00712_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/ec9f536d1e6e/ct4c00712_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/db619b75c029/ct4c00712_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/5b31c176e968/ct4c00712_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cd8f/11325537/86864985b97b/ct4c00712_0005.jpg

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