Lykhin Aleksandr O, Truhlar Donald G, Gagliardi Laura
Department of Chemistry, Pritzker School of Molecular Engineering, The James Franck Institute and Chicago Center for Theoretical Chemistry, The University of Chicago, Chicago, Illinois 60637, United States.
Department of Chemistry, Chemical Theory Center, and Minnesota Supercomputing Institute, University of Minnesota, Minneapolis, Minnesota 55455, United States.
J Chem Theory Comput. 2021 Dec 14;17(12):7586-7601. doi: 10.1021/acs.jctc.1c00915. Epub 2021 Nov 18.
The dipole moment is the molecular property that most directly indicates molecular polarity. The accuracy of computed dipole moments depends strongly on the quality of the calculated electron density, and the breakdown of single-reference methods for strongly correlated systems can lead to poor predictions of the dipole moments in those cases. Here, we derive the analytical expression for obtaining the electric dipole moment by multiconfiguration pair-density functional theory (MC-PDFT), and we assess the accuracy of MC-PDFT for predicting dipole moments at equilibrium and nonequilibrium geometries. We show that MC-PDFT dipole moment curves have reasonable behavior even for stretched geometries, and they significantly improve upon the CASSCF results by capturing more electron correlation. The analysis of a dataset consisting of 18 first-row transition-metal diatomics and 6 main-group polyatomic molecules with a multireference character suggests that MC-PDFT and its hybrid extension (HMC-PDFT) perform comparably to CASPT2 and MRCISD+Q methods and have a mean unsigned deviation of 0.2-0.3 D with respect to the best available dipole moment reference values. We explored the dependence of the predicted dipole moments upon the choice of the on-top density functional and active space, and we recommend the tPBE and hybrid tPBE0 on-top choices for the functionals combined with the moderate correlated-participating-orbitals scheme for selecting the active space. With these choices, the mean unsigned deviations (in debyes) of the calculated equilibrium dipole moments from the best estimates are 0.77 for CASSCF, 0.29 for MC-PDFT, 0.24 for HMC-PDFT, 0.28 for CASPT2, and 0.25 for MRCISD+Q. These results are encouraging because the computational cost of MC-PDFT or HMC-PDFT is largely reduced compared to the CASPT2 and MRCISD+Q methods.
偶极矩是最直接表明分子极性的分子性质。计算得到的偶极矩的准确性在很大程度上取决于所计算电子密度的质量,对于强相关体系,单参考方法的失效会导致在这些情况下对偶极矩的预测不佳。在此,我们推导了通过多组态对密度泛函理论(MC-PDFT)获得电偶极矩的解析表达式,并评估了MC-PDFT在预测平衡和非平衡几何构型下偶极矩时的准确性。我们表明,即使对于拉伸几何构型,MC-PDFT偶极矩曲线也具有合理的行为,并且通过捕捉更多的电子相关性,它们在CASSCF结果的基础上有显著改进。对由18个第一行过渡金属双原子分子和6个具有多参考特征的主族多原子分子组成的数据集的分析表明,MC-PDFT及其混合扩展(HMC-PDFT)的表现与CASPT2和MRCISD+Q方法相当,相对于最佳可用偶极矩参考值,平均无符号偏差为0.2 - 0.3 D。我们探讨了预测偶极矩对顶密度泛函和活性空间选择的依赖性,并推荐tPBE和混合tPBE0顶密度泛函选择,以及适度的相关参与轨道方案来选择活性空间。采用这些选择时,计算得到的平衡偶极矩与最佳估计值的平均无符号偏差(单位为德拜),CASSCF为0.77,MC-PDFT为0.29,HMC-PDFT为为0.24,CASPT2为0.28,MRCISD+Q为0.25。这些结果令人鼓舞,因为与CASPT2和MRCISD+Q方法相比,MC-PDFT或HMC-PDFT的计算成本大幅降低。