Xu Peng, Leonard Samuel L, O'Brien William, Gordon Mark S
Department of Chemistry, Iowa State University and Ames National Laboratory, Ames, Iowa 50014, United States.
Science Undergraduate Research Internship (SULI): Department of Energy, Ames National Laboratory, Iowa State University, Ames, Iowa50011-3020, United States.
J Phys Chem A. 2024 Jan 11;128(1):292-327. doi: 10.1021/acs.jpca.3c05115. Epub 2023 Dec 27.
The anisotropic and isotropic R dispersion contributions (disp8) are derived and implemented within the framework of the effective fragment potential (EFP) method formulated with imaginary frequency-dependent Cartesian polarizability tensors distributed at the centroids of the localized molecular orbitals (LMOs). Two forms of damping functions, intermolecular overlap-based and Tang-Toennies, are extended for disp8. To obtain LMO polarizability tensors centered at LMO centroids, an origin-shifting transformation is derived and implemented for the dipole-octopole polarizability tensor and the quadrupole-quadrupole polarizability tensor. The analytic gradient is derived and implemented for the isotropic disp8 contribution. Relative to the previously implemented empirical EFP disp8 energy, the isotropic disp8 component of the interaction energy improves the overall agreement of the EFP dispersion energies with the symmetry-adapted perturbation theory (SAPT) benchmarks, reducing the mean absolute errors (MAEs) and mean absolute percentage errors for most of the databases examined in this work. While the anisotropic disp8 can further enhance the accuracy of the EFP dispersion energy and yield smaller MAEs, significantly overbound dispersion energies are predicted by the anisotropic disp8 when the maximum element in the intermolecular overlap matrix is greater than 0.1, possibly due to the breakdown of the approximations made in the EFP dispersion derivation at a short range. For potential energy scan databases, the newly developed EFP dispersion model with isotropic disp8 yields the overall correct curvature and good agreement with SAPT benchmarks around equilibrium and longer but overestimates the dispersion interactions at a short range. While the overlap-based dispersion-damping functions produce better MAEs than Tang-Toennies damping functions, further improvement is needed to better screen the large attractive dispersion energies at a short range (overlap >0.1).
在有效片段势(EFP)方法框架内,基于分布在定域分子轨道(LMO)质心处的与虚频相关的笛卡尔极化率张量,推导并实现了各向异性和各向同性的R色散贡献(disp8)。为disp8扩展了两种形式的阻尼函数,即基于分子间重叠的阻尼函数和Tang-Toennies阻尼函数。为了获得以LMO质心为中心的LMO极化率张量,推导并实现了针对偶极-八极极化率张量和四极-四极极化率张量的原点平移变换。推导并实现了各向同性disp8贡献的解析梯度。相对于先前实现的经验性EFP disp8能量,相互作用能的各向同性disp8分量提高了EFP色散能量与对称适配微扰理论(SAPT)基准的整体一致性,降低了本工作中所研究的大多数数据库的平均绝对误差(MAE)和平均绝对百分比误差。虽然各向异性disp8可以进一步提高EFP色散能量的精度并产生更小的MAE,但当分子间重叠矩阵中的最大元素大于0.1时,各向异性disp8会预测出明显过度束缚的色散能量,这可能是由于在短程EFP色散推导中所做近似的失效。对于势能扫描数据库,新开发的具有各向同性disp8的EFP色散模型在平衡附近和较长距离处产生了总体正确的曲率并且与SAPT基准吻合良好,但在短程处高估了色散相互作用。虽然基于重叠的色散阻尼函数产生的MAE比Tang-Toennies阻尼函数更好,但仍需要进一步改进以更好地筛选短程(重叠>0.1)处大的吸引性色散能量。