Division of Theoretical Chemistry, Lund University , P.O. Box 124, 221 00 Lund, Sweden.
J Chem Theory Comput. 2016 Apr 12;12(4):1647-55. doi: 10.1021/acs.jctc.6b00034. Epub 2016 Mar 10.
The chromium dimer has long been a benchmark molecule to evaluate the performance of different computational methods ranging from density functional theory to wave function methods. Among the latter, multiconfigurational perturbation theory was shown to be able to reproduce the potential energy surface of the chromium dimer accurately. However, for modest active space sizes, it was later shown that different definitions of the zeroth-order Hamiltonian have a large impact on the results. In this work, we revisit the system for the third time with multiconfigurational perturbation theory, now in order to increase the active space of the reference wave function. This reduces the impact of the choice of zeroth-order Hamiltonian and improves the shape of the potential energy surface significantly. We conclude by comparing our results of the dissocation energy and vibrational spectrum to those obtained from several highly accurate multiconfigurational methods and experiment. For a meaningful comparison, we used the extrapolation to the complete basis set for all methods involved.
铬二聚体长期以来一直是评估从密度泛函理论到波函数方法等不同计算方法性能的基准分子。在后者中,多组态微扰理论被证明能够准确地再现铬二聚体的势能面。然而,对于适度的活动空间大小,后来表明零阶哈密顿量的不同定义对结果有很大的影响。在这项工作中,我们第三次使用多组态微扰理论重新研究该系统,现在是为了增加参考波函数的活动空间。这减少了零阶哈密顿量选择的影响,并显著改善了势能面的形状。我们最后通过将离解能和振动光谱的结果与从几种高精度多组态方法和实验中获得的结果进行比较来得出结论。为了进行有意义的比较,我们对所有涉及的方法都使用了完全基组的外推。