Karton Amir
School of Molecular Sciences, The University of Western Australia, Perth, WA 6009, Australia.
J Chem Phys. 2020 Jul 14;153(2):024102. doi: 10.1063/5.0011674.
It is well established that extrapolating the coupled-cluster single double triple [CCSD and (T)] correlation energies using empirically motivated extrapolation exponents can accelerate the basis set convergence. Here, we consider the extrapolation of coupled-cluster expansion terms beyond the CCSD(T) level to the complete basis set (CBS) limit. We obtain reference CCSDT-CCSD(T) [T-(T)], CCSDT(Q)-CCSDT [(Q)], and CCSDTQ-CCSDT(Q) [T-(Q)] contributions from cc-pV{5,6}Z extrapolations for a diverse set of 16 first- and second-row systems. We use these basis-set limit results to fit extrapolation exponents in conjunction with the cc-pV{D,T}Z, cc-pV{T,Q}Z, and cc-pV{Q,5}Z basis set pairs. The optimal extrapolation exponents result in noticeable improvements in performance (relative to α = 3.0) in conjunction with the cc-pV{T,Q}Z basis set pair; however, smaller improvements are obtained for the other basis sets. These results confirm that the basis sets and basis set extrapolations used for obtaining post-CCSD(T) components in composite thermochemical theories such as Weizmann-4 and HEAT are sufficiently close to the CBS limit for attaining sub-kJ/mole accuracy. The fitted extrapolation exponents demonstrate that the T-(T) correlation component converges more slowly to the CBS limit than the (Q) and T terms. A systematic investigation of the effect of diffuse functions shows that it diminishes (i) in the order T-(T) > (Q) > T-(Q) and (ii) with the size of the basis set. Importantly, we find that diffuse functions tend to systematically reduce the T-(T) contribution but systematically increases the (Q) contribution. Thus, the use of the cc-pVnZ basis sets benefits from a certain degree of error cancellation between these two components.
众所周知,使用基于经验的外推指数来外推耦合簇单双三激发 [CCSD 和 (T)] 相关能,可以加速基组收敛。在此,我们考虑将耦合簇展开项从 CCSD(T) 水平外推到完备基组 (CBS) 极限。对于 16 个不同的第一和第二周期体系,我们从 cc-pV{5,6}Z 外推中获得了参考 CCSDT-CCSD(T) [T-(T)]、CCSDT(Q)-CCSDT [(Q)] 和 CCSDTQ-CCSDT(Q) [T-(Q)] 贡献。我们使用这些基组极限结果,结合 cc-pV{D,T}Z、cc-pV{T,Q}Z 和 cc-pV{Q,5}Z 基组对来拟合外推指数。与 cc-pV{T,Q}Z 基组对结合使用时,最优外推指数在性能上(相对于 α = 3.0)有显著提升;然而,对于其他基组,提升较小。这些结果证实,在诸如魏茨曼 - 4 和 HEAT 等复合热化学理论中,用于获得 CCSD(T) 后成分的基组和基组外推足够接近 CBS 极限,以达到亚千焦/摩尔的精度。拟合的外推指数表明,T-(T) 相关分量比 (Q) 和 T 项更慢地收敛到 CBS 极限。对弥散函数效应的系统研究表明,它按以下顺序减小:(i) T-(T) > (Q) > T-(Q),以及 (ii) 随着基组大小的增加而减小。重要的是,我们发现弥散函数倾向于系统地降低 T-(T) 贡献,但系统地增加 (Q) 贡献。因此,使用 cc-pVnZ 基组受益于这两个分量之间一定程度的误差抵消。