Chen Zehua, Zhang Du, Jin Ye, Yang Yang, Su Neil Qiang, Yang Weitao
Department of Chemistry, Duke University , Durham, North Carolina 27708, United States.
J Phys Chem Lett. 2017 Sep 21;8(18):4479-4485. doi: 10.1021/acs.jpclett.7b01864. Epub 2017 Sep 6.
To describe static correlation, we develop a new approach to density functional theory (DFT), which uses a generalized auxiliary system that is of a different symmetry, such as particle number or spin, from that of the physical system. The total energy of the physical system consists of two parts: the energy of the auxiliary system, which is determined with a chosen density functional approximation (DFA), and the excitation energy from an approximate linear response theory that restores the symmetry to that of the physical system, thus rigorously leading to a multideterminant description of the physical system. The electron density of the physical system is different from that of the auxiliary system and is uniquely determined from the functional derivative of the total energy with respect to the external potential. Our energy functional is thus an implicit functional of the physical system density, but an explicit functional of the auxiliary system density. We show that the total energy minimum and stationary states, describing the ground and excited states of the physical system, can be obtained by a self-consistent optimization with respect to the explicit variable, the generalized Kohn-Sham noninteracting density matrix. We have developed the generalized optimized effective potential method for the self-consistent optimization. Among options of the auxiliary system and the associated linear response theory, reformulated versions of the particle-particle random phase approximation (pp-RPA) and the spin-flip time-dependent density functional theory (SF-TDDFT) are selected for illustration of principle. Numerical results show that our multireference DFT successfully describes static correlation in bond dissociation and double bond rotation.
为了描述静态关联,我们开发了一种新的密度泛函理论(DFT)方法,该方法使用一个广义辅助系统,其对称性(如粒子数或自旋)与物理系统不同。物理系统的总能量由两部分组成:辅助系统的能量,它由选定的密度泛函近似(DFA)确定;以及来自近似线性响应理论的激发能,该理论将对称性恢复到物理系统的对称性,从而严格地得到物理系统的多行列式描述。物理系统的电子密度与辅助系统的不同,并且由总能量相对于外部势的泛函导数唯一确定。因此,我们的能量泛函是物理系统密度的隐式泛函,但却是辅助系统密度的显式泛函。我们表明,描述物理系统基态和激发态的总能量最小值和定态,可以通过对显式变量——广义Kohn-Sham非相互作用密度矩阵进行自洽优化来获得。我们已经开发了用于自洽优化的广义优化有效势方法。在辅助系统和相关线性响应理论的选项中,选择了粒子-粒子随机相位近似(pp-RPA)和自旋翻转含时密度泛函理论(SF-TDDFT)的重新表述版本来说明原理。数值结果表明,我们的多参考DFT成功地描述了键解离和双键旋转中的静态关联。