Department of Chemistry , The University of Western Ontario , London , Ontario N6A 5B7 , Canada.
J Chem Theory Comput. 2019 Sep 10;15(9):4956-4964. doi: 10.1021/acs.jctc.9b00618. Epub 2019 Aug 22.
Calculation of vertical excitation energies by the adiabatic linear-response time-dependent density-functional theory (TDDFT) requires static Kohn-Sham potentials and exchange-correlation kernels. When these quantities are derived from standard density-functional approximations (DFA), mean absolute errors (MAE) of the method are known to range from 0.2 eV to over 1 eV, depending on the functional and type of excitation. We investigate how the performance of TDDFT varies when increasingly accurate exchange-correlation potentials derived from Hartree-Fock (HF) and post-HF wavefunctions are combined with different approximate kernels. The lowest MAEs obtained in this manner for valence excitations are about 0.15-0.2 eV, which appears to be the practical limit of the accuracy of TDDFT that can be achieved by improving the Kohn-Sham potentials alone. These findings are consistent with previous reports on the benefits of accurate exchange-correlation potentials in TDDFT, but provide new insights and afford more definitive conclusions.
通过绝热线性响应时间相关密度泛函理论(TDDFT)计算垂直激发能需要静态 Kohn-Sham 势和交换相关核。当这些量由标准密度泛函近似(DFA)得出时,该方法的平均绝对误差(MAE)已知在 0.2 eV 到 1 eV 以上之间变化,具体取决于功能和激发类型。我们研究了随着越来越精确的 Hartree-Fock(HF)和后 Hartree-Fock 波函数导出的交换相关势与不同的近似核相结合,TDDFT 的性能如何变化。以这种方式获得的价激发的最低 MAE 约为 0.15-0.2 eV,这似乎是仅通过改进 Kohn-Sham 势就可以实现的 TDDFT 精度的实际极限。这些发现与之前关于 TDDFT 中准确交换相关势的好处的报告一致,但提供了新的见解并得出了更明确的结论。