Density functional theory‐based rapid and accurate estimation of reduction potentials of acridinium derivatives in ground and excited state

Author:

Choi Jiyoon1,Kang Kyungtae2,Park Ji Hun3ORCID,Kim Hyungjun1ORCID

Affiliation:

1. Department of Chemistry and Research Institute of Basic Sciences Incheon National University Incheon Republic of Korea

2. Department of Applied Chemistry Kyung Hee University Yongin‐Si Gyeonggi‐do Republic of Korea

3. Department of Science Education Ewha Womans University Seoul Republic of Korea

Abstract

AbstractWe devised a quantum chemical simulation protocol that can rapidly and accurately predict ground and excited state reduction potentials (E0 and E*, respectively) of acridinium photoredox catalysts (PCs). To bypass time‐consuming excited state geometry optimizations, we used ground state equilibrium geometries to compute the electronic energy of excited states, which provides reasonable E0 and E* estimates. The contribution of Hartree‐Fock exchange (HFX) in density functionals was systematically varied to estimate E0 and E*. In addition to reproducing experimental results, physically sensible models, such as correct descriptions of exciton behavior, are highly necessary. Based on the exciton correlation values, the appropriate amount of HFX in the B3LYP functional was determined to be 30 % to yield physically sensible bound electron‐hole pairs for small organic molecules. We also investigated the impact of basis sets on the predictability of E0 and E*. Geometry optimizations with B3LYP‐D2(HFX 20 %)/6‐31G and single point energy refinement with (TD‐)B3LYP‐D2(HFX 30%)/6‐311++G(d,p) yielded the best results. The transferability of the suggested protocol was confirmed with a test set consisting of eight acridinium derivatives. This study can provide reasonably accurate results with relatively small amounts of computational resources, and it is therefore expected to greatly contribute to the development of new acridinium PCs.

Funder

Incheon National University

Publisher

Wiley

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