Department of Chemistry, Duke University, Durham, North Carolina 27708, USA.
J Chem Phys. 2017 Oct 7;147(13):134105. doi: 10.1063/1.4994827.
The optimized effective potential (OEP) that gives accurate Kohn-Sham (KS) orbitals and orbital energies can be obtained from a given reference electron density. These OEP-KS orbitals and orbital energies are used here for calculating electronic excited states with the particle-particle random phase approximation (pp-RPA). Our calculations allow the examination of pp-RPA excitation energies with the exact KS density functional theory (DFT). Various input densities are investigated. Specifically, the excitation energies using the OEP with the electron densities from the coupled-cluster singles and doubles method display the lowest mean absolute error from the reference data for the low-lying excited states. This study probes into the theoretical limit of the pp-RPA excitation energies with the exact KS-DFT orbitals and orbital energies. We believe that higher-order correlation contributions beyond the pp-RPA bare Coulomb kernel are needed in order to achieve even higher accuracy in excitation energy calculations.
可以从给定的参考电子密度中获得提供准确 Kohn-Sham(KS)轨道和轨道能量的优化有效势(OEP)。 这里使用这些 OEP-KS 轨道和轨道能量来计算具有粒子-粒子随机相位近似(pp-RPA)的电子激发态。 我们的计算允许用精确的 KS 密度泛函理论(DFT)检查 pp-RPA 激发能。 研究了各种输入密度。 具体来说,使用与耦合簇单双方法的电子密度相对应的 OEP 计算的激发能,对于低能激发态,其与参考数据的平均绝对误差最小。 这项研究探讨了使用精确 KS-DFT 轨道和轨道能量的 pp-RPA 激发能的理论极限。 我们认为,需要超越 pp-RPA 裸库仑核的更高阶相关贡献,才能在激发能计算中实现更高的精度。