Fujita Takatoshi, Noguchi Yoshifumi
Institute for Quantum Life Science, National Institutes for Quantum Science and Technology, Tokai, Ibaraki 319-1106, Japan.
Department of Applied Chemistry and Biochemical Engineering, Graduate School of Engineering, Shizuoka University, Hamamatsu, Shizuoka 432-8561, Japan.
J Phys Chem A. 2021 Dec 16;125(49):10580-10592. doi: 10.1021/acs.jpca.1c07337. Epub 2021 Dec 6.
Herein, we present a fragment-based approach for calculating the charged and neutral excited states in molecular systems, based on the many-body Green's function method within the GW approximation and the Bethe-Salpeter equation (BSE). The implementation relies on the many-body expansion of the total irreducible polarizability on the basis of fragment molecular orbitals. The GW quasi-particle energies in complex molecular environments are obtained by the GW calculation for the target fragment plus induced polarization contributions of the surrounding fragments at the static Coulomb-hole plus screened exchange level. In addition, we develop a large-scale GW/BSE method for calculating the delocalized excited states of molecular aggregates, based on the fragment molecular orbital method and the exciton model. The accuracy of fragment-based GW and GW/BSE methods was evaluated on molecular clusters and molecular crystals. We found that the accuracy of the total irreducible polarizability can be improved systematically by including two-body correction terms, and the fragment-based calculations can reasonably reproduce the results of the corresponding unfragmented calculations with a relative error of less than 100 meV. The proposed approach enables efficient excited-state calculations for large molecular systems with reasonable accuracy.
在此,我们基于GW近似下的多体格林函数方法和贝叶斯-萨尔皮特方程(BSE),提出了一种用于计算分子体系中带电和中性激发态的基于片段的方法。该实现依赖于基于片段分子轨道的总不可约极化率的多体展开。通过对目标片段进行GW计算,并加上周围片段在静态库仑空穴加屏蔽交换水平上的诱导极化贡献,可得到复杂分子环境中的GW准粒子能量。此外,我们基于片段分子轨道方法和激子模型,开发了一种用于计算分子聚集体离域激发态的大规模GW/BSE方法。在分子簇和分子晶体上评估了基于片段的GW和GW/BSE方法的准确性。我们发现,通过包含两体校正项,可以系统地提高总不可约极化率的准确性,并且基于片段的计算能够以小于100 meV的相对误差合理地重现相应的无片段计算结果。所提出的方法能够以合理的准确性对大分子体系进行高效的激发态计算。