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Toward a less costly but accurate calculation of the CCSD(T)/CBS noncovalent interaction energy
Author(s) -
Chen JiuLi,
Sun Tao,
Wang YiBo,
Wang Weizhou
Publication year - 2020
Publication title -
journal of computational chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.907
H-Index - 188
eISSN - 1096-987X
pISSN - 0192-8651
DOI - 10.1002/jcc.26171
Subject(s) - coupled cluster , basis set , perturbation theory (quantum mechanics) , term (time) , chemistry , physics , atomic physics , computational chemistry , quantum mechanics , density functional theory , molecule
Abstract The popular method of calculating the noncovalent interaction energies at the coupled‐cluster single‐, double‐, and perturbative triple‐excitations [CCSD(T)] theory level in the complete basis set (CBS) limit was to add a CCSD(T) correction term to the CBS second‐order Møller‐Plesset perturbation theory (MP2). The CCSD(T) correction term is the difference between the CCSD(T) and MP2 interaction energies evaluated in a medium basis set. However, the CCSD(T) calculations with the medium basis sets are still very expensive for systems with more than 30 atoms. Comparatively, the domain‐based local pair natural orbital coupled‐cluster method [DLPNO‐CCSD(T)] can be applied to large systems with over 1,000 atoms. Considering both the computational accuracy and efficiency, in this work, we propose a new scheme to calculate the CCSD(T)/CBS interaction energies. In this scheme, the MP2/CBS term keeps intact and the CCSD(T) correction term is replaced by a DLPNO‐CCSD(T) correction term which is the difference between the DLPNO‐CCSD(T) and DLPNO‐MP2 interaction energies evaluated in a medium basis set. The interaction energies of the noncovalent systems in the S22, HSG, HBC6, NBC10, and S66 databases were recalculated employing this new scheme. The consistent and tight settings of the truncation parameters for DLPNO‐CCSD(T) and DLPNO‐MP2 in this noncanonical CCSD(T)/CBS calculations lead to the maximum absolute deviation and root‐mean‐square deviation from the canonical CCSD(T)/CBS interaction energies of less than or equal to 0.28 kcal/mol and 0.09 kcal/mol, respectively. The high accuracy and low cost of this new computational scheme make it an excellent candidate for the study of large noncovalent systems.