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弥合基于变分和微扰密度泛函理论方法在计算激发态方面的差距。

Bridging the Gap between Variational and Perturbational DFT-Based Methods for Calculating Excited States.

作者信息

Sinyavskiy Andrey, Mališ Momir, Luber Sandra

机构信息

Department of Chemistry, University of Zurich, Winterthurerstrasse 190, 8057 Zürich, Switzerland.

出版信息

J Chem Theory Comput. 2025 Aug 12;21(15):7430-7449. doi: 10.1021/acs.jctc.5c00724. Epub 2025 Jul 22.

Abstract

A thorough investigation of the delta self-consistent field (ΔSCF) method within the restricted-open Kohn-Sham (ROKS) formalism has been carried out. The ROKS-based ΔSCF targets unmixed singlet excited electronic states, avoiding the need for a spin purification procedure. A modification of the maximum overlap method to improve the convergence of the ΔSCF method is presented, in addition to a molecular orbital tracking and order-preserving algorithm. For benchmarking purposes a large-scale comparison with time-dependent density functional theory (TDDFT) was conducted: both single- and multi-reference singlet and triplet excited electronic states of various molecules were reproduced using ΔSCF and compared to the states provided by TDDFT. Besides the excitation energies, we also compared the electron densities and the transition dipole moments of the molecules between the two methods.

摘要

对受限开壳层Kohn-Sham(ROKS)形式体系中的δ自洽场(ΔSCF)方法进行了全面研究。基于ROKS的ΔSCF针对未混合的单重激发电子态,无需自旋纯化程序。除了分子轨道跟踪和保序算法外,还提出了一种改进的最大重叠方法以提高ΔSCF方法的收敛性。为了进行基准测试,与含时密度泛函理论(TDDFT)进行了大规模比较:使用ΔSCF再现了各种分子的单重和多重参考单重态和三重激发电子态,并与TDDFT提供的态进行了比较。除了激发能之外,我们还比较了两种方法之间分子的电子密度和跃迁偶极矩。

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