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通过直接优化进行激发态的变分密度泛函计算。

Variational Density Functional Calculations of Excited States via Direct Optimization.

作者信息

Levi Gianluca, Ivanov Aleksei V, Jónsson Hannes

机构信息

Science Institute and Faculty of Physical Sciences, University of Iceland, 107 Reykjavík, Iceland.

Saint Petersburg State University, 199034 Saint Petersburg, Russia.

出版信息

J Chem Theory Comput. 2020 Nov 10;16(11):6968-6982. doi: 10.1021/acs.jctc.0c00597. Epub 2020 Oct 16.

Abstract

The development of variational density functional theory approaches to excited electronic states is impeded by limitations of the commonly used self-consistent field (SCF) procedure. A method based on a direct optimization approach as well as the maximum overlap method is presented, and the performance is compared with previously proposed SCF strategies. Excited-state solutions correspond to saddle points of the energy as a function of the electronic degrees of freedom. The approach presented here makes use of a preconditioner determined with the help of the maximum overlap method to guide the convergence on a target th-order saddle point. This method is found to be more robust and converge faster than previously proposed SCF approaches for a set of 89 excited states of molecules. A limited-memory formulation of the symmetric rank-one method for updating the inverse Hessian is found to give the best performance. A conical intersection for the carbon monoxide molecule is calculated without resorting to fractional occupation numbers. Calculations on the excited states of the hydrogen atom and a doubly excited state of the dihydrogen molecule using a self-interaction corrected functional are presented. For these systems, the self-interaction correction is found to improve the accuracy of density functional calculations of excited states.

摘要

变分密度泛函理论方法在激发电子态方面的发展受到常用自洽场(SCF)程序局限性的阻碍。本文提出了一种基于直接优化方法以及最大重叠方法的方法,并将其性能与先前提出的SCF策略进行了比较。激发态解对应于能量作为电子自由度函数的鞍点。这里提出的方法利用借助最大重叠方法确定的预处理器来引导在目标第(n)阶鞍点上的收敛。对于一组89个分子激发态,发现该方法比先前提出的SCF方法更稳健且收敛更快。发现用于更新逆海森矩阵的对称秩一方法的有限内存公式给出了最佳性能。在不借助分数占据数的情况下计算了一氧化碳分子的锥形交叉点。给出了使用自相互作用校正泛函对氢原子激发态和双原子分子双激发态的计算结果。对于这些体系,发现自相互作用校正提高了激发态密度泛函计算的准确性。

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