McKeon Caroline A, Hamed Samia M, Bruneval Fabien, Neaton Jeffrey B
Department of Physics, University of California, Berkeley, California 94720, USA.
Université Paris-Saclay, CEA, Service de Recherches de Métallurgie Physique, 91191 Gif-sur-Yvette, France.
J Chem Phys. 2022 Aug 21;157(7):074103. doi: 10.1063/5.0097582.
The ab initio GW plus Bethe-Salpeter equation (GW-BSE, where G is the one particle Green's function and W is the screened Coulomb interaction) approach has emerged as a leading method for predicting excitations in both solids and molecules with a predictive power contingent upon several factors. Among these factors are the (1) generalized Kohn-Sham eigensystem used to construct the GW self-energy and to solve the BSE and (2) the efficacy and suitability of the Tamm-Dancoff approximation. Here, we present a detailed benchmark study of low-lying singlet excitations from a generalized Kohn-Sham (gKS) starting point based on an optimally tuned range-separated hybrid (OTRSH) functional. We show that the use of this gKS starting point with one-shot GW and GW-BSE leads to the lowest mean absolute errors (MAEs) and mean signed errors (MSEs), with respect to high-accuracy reference values, demonstrated in the literature thus far for the ionization potentials of the GW100 benchmark set and for low-lying neutral excitations of Thiel's set molecules in the gas phase, without the need for self-consistency. The MSEs and MAEs of one-shot GW-BSE@OTRSH excitation energies are comparable to or lower than those obtained with other functional starting points after self-consistency. Additionally, we compare these results with linear-response time-dependent density functional theory (TDDFT) calculations and find GW-BSE to be superior to TDDFT when calculations are based on the same exchange-correlation functional. This work demonstrates tuned range-separated hybrids used in combination with GW and GW-BSE can greatly suppress starting point dependence for molecules, leading to accuracy similar to that for higher-order wavefunction-based theories for molecules without the need for costlier iterations to self-consistency.
从头算GW加贝塞耳-萨尔皮特方程(GW-BSE,其中G是单粒子格林函数,W是屏蔽库仑相互作用)方法已成为预测固体和分子激发的领先方法,其预测能力取决于几个因素。这些因素包括:(1)用于构建GW自能和求解BSE的广义科恩-沙姆本征系统,以及(2)塔姆-丹科夫近似的有效性和适用性。在此,我们基于最优调谐的范围分离杂化(OTRSH)泛函,从广义科恩-沙姆(gKS)起点出发,对低能单重激发进行了详细的基准研究。我们表明,对于GW100基准集的电离势以及气相中蒂尔集分子的低能中性激发,使用这种gKS起点结合单次GW和GW-BSE,相对于迄今为止文献中展示的高精度参考值,能产生最低的平均绝对误差(MAE)和平均符号误差(MSE),且无需自洽。单次GW-BSE@OTRSH激发能的MSE和MAE与自洽后使用其他泛函起点获得的结果相当或更低。此外,我们将这些结果与线性响应含时密度泛函理论(TDDFT)计算进行比较,发现当基于相同的交换关联泛函进行计算时,GW-BSE优于TDDFT。这项工作表明,与GW和GW-BSE结合使用的调谐范围分离杂化方法可以极大地抑制分子的起点依赖性,在无需进行更昂贵的自洽迭代的情况下,产生与基于高阶波函数的分子理论相似的精度。