Department of Chemistry and Biochemistry , The Ohio State University , Columbus , Ohio 43210 , United States.
J Chem Theory Comput. 2018 Jun 12;14(6):2955-2978. doi: 10.1021/acs.jctc.8b00058. Epub 2018 May 2.
We report an implementation of extended symmetry-adapted perturbation theory (XSAPT) in the atomic orbital basis, extending this method to systems where the monomers are large. In our "XSAPT(KS)" approach, monomers are described using range-separated Kohn-Sham (KS) density functional theory (DFT), with correct asymptotic behavior set by tuning the range-separation parameter ω in a monomer-specific way. This is accomplished either by conventional ionization potential (IP)-based tuning, in which ω is adjusted to satisfy the condition ε(ω) = -IP(ω), or else using a "global density-dependent" (GDD) condition, in which ω is fixed based on the size of the exchange hole. The latter procedure affords better results for both total interaction energies and energy components, when used in conjunction with our third-generation pairwise atom-atom dispersion potential (+ aiD3). Three-body (triatomic) dispersion terms are found to be important when the monomers are large, and we incorporate these by means of an Axilrod-Teller-Muto term, E, which reduces errors in supramolecular interaction energies by about a factor of 2. The XSAPT(KS) + aiD3 + E(ω) approach affords mean absolute errors as low as 1.2 and 4.2 kcal/mol, respectively, for the L7 and S12L benchmark test sets of large dimers. Such errors are comparable to those afforded by far more expensive methods, such as DFT-SAPT, and the closely related second-order perturbation theory with coupled dispersion (MP2C). We also survey the performance of various other quantum-chemical methods for these data sets and identify several semiempirical and DFT-based approaches whose accuracy approaches that of MP2C, at dramatically reduced cost.
我们报告了在原子轨道基下扩展的对称性自适应微扰理论(XSAPT)的实现,将该方法扩展到单体较大的系统中。在我们的“XSAPT(KS)”方法中,单体使用范围分离的 Kohn-Sham(KS)密度泛函理论(DFT)来描述,通过单体特定的方式调整范围分离参数ω来设置正确的渐近行为。这可以通过传统的电离势(IP)基调谐来完成,其中ω被调整以满足条件 ε(ω) = -IP(ω),或者使用“全局密度相关”(GDD)条件,其中ω基于交换孔的大小来固定。当与我们的第三代原子间对分散势(+ aiD3)结合使用时,后一种方法在总相互作用能和能量分量方面都能产生更好的结果。当单体较大时,三体(三原子)分散项变得很重要,我们通过 Axilrod-Teller-Muto 项 E 来包含这些项,E 项通过将超分子相互作用能的误差降低约 2 倍。对于较大的二聚体的 L7 和 S12L 基准测试集,XSAPT(KS) + aiD3 + E(ω)方法的平均绝对误差分别低至 1.2 和 4.2 kcal/mol。这些误差与更昂贵的方法(如 DFT-SAPT)和密切相关的二阶微扰理论与耦合分散(MP2C)提供的误差相当。我们还调查了这些数据集的各种其他量子化学方法的性能,并确定了几种半经验和基于 DFT 的方法,其准确性接近 MP2C,成本却大大降低。