Affiliation:
1. Fukui Institute for Fundamental Chemistry Kyoto University Kyoto Japan
2. RIKEN Center for Computational Science Kobe Japan
3. Graduate School of Engineering Nagasaki University Nagasaki Japan
4. Department of Natural Sciences Southwest Tennessee Community College Memphis Tennessee USA
Abstract
AbstractThe core ionization energies of second‐ and third‐period elements of the molecules C2H5NO2, SiF4, Si(CH3)4, PF3, POF3, PSF3, CS2, OCS, SO2, SO2F2, CH3Cl, CFCl3, SF5Cl, and Cl3PS are calculated by using Hartree‐Fock (HF), and Kohn‐Sham (KS) with BH&HLYP, B3LYP, and LC‐BOP functionals. We used ΔSCF, Slater's transition state (STS), and two previously proposed shifted STS (1) and shifted STS (2) methods, which have been developed. The errors of ΔSCF and STS come mainly from the self‐interaction errors (SIE) and can be corrected with a shifting scheme. In this study, we used the shifting parameters determined for each atom. The shifted STS (1) reproduces ΔSCF almost perfectly with mean absolute deviations (MAD) of 0.02 eV. While ΔSCF and STS vary significantly depending on the functional used, the variation of shifted STS (2) is small, and all shifted STS (2) values are close to the observed ones. The deviations of the shifted STS (2) from the experiment are 0.24 eV (BH&HLYP), 0.19 eV (B3LYP), and 0.23 eV (LC‐BOP). These results further support the use of shifted STS methods for predicting the core ionization energies.
Funder
Hyogo Science and Technology Association
Ministry of Science and ICT, South Korea
Subject
Computational Mathematics,General Chemistry
Cited by
3 articles.
订阅此论文施引文献
订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献