ImprovedSCF interaction energy decomposition scheme corrected for basis set superposition effect

1983 ◽  
Vol 23 (3) ◽  
pp. 847-854 ◽  
Author(s):  
W. A. Sokalski ◽  
S. Roszak ◽  
P. C. Hariharan ◽  
Joyce J. Kaufman
2014 ◽  
Vol 119 (29) ◽  
pp. 9056-9067 ◽  
Author(s):  
Marwa H. Farag ◽  
Manuel F. Ruiz-López ◽  
Adolfo Bastida ◽  
Gérald Monard ◽  
Francesca Ingrosso

Molecules ◽  
2021 ◽  
Vol 26 (18) ◽  
pp. 5526
Author(s):  
Iván González-Veloso ◽  
Nádia M. Figueiredo ◽  
M. Natália D. S. Cordeiro

This work aims at unravelling the interactions in magnetic ionic liquids (MILs) by applying Symmetry-Adapted Perturbation Theory (SAPT) calculations, as well as based on those to set-up a polarisable force field model for these liquids. The targeted MILs comprise two different cations, namely: 1-butyl-3-methylimidazolium ([Bmim]+) and 1-ethyl-3-methylimidazolium ([Emim]+), along with several metal halides anions such as [FeCl4]−, [FeBr4]−, [ZnCl3]− and [SnCl4]2− To begin with, DFT geometry optimisations of such MILs were performed, which in turn revealed that the metallic anions prefer to stay close to the region of the carbon atom between the nitrogen atoms in the imidazolium fragment. Then, a SAPT study was carried out to find the optimal separation of the monomers and the different contributions for their interaction energy. It was found that the main contribution to the interaction energy is the electrostatic interaction component, followed by the dispersion one in most of the cases. The SAPT results were compared with those obtained by employing the local energy decomposition scheme based on the DLPNO-CCSD(T) method, the latter showing slightly lower values for the interaction energy as well as an increase of the distance between the minima centres of mass. Finally, the calculated SAPT interaction energies were found to correlate well with the melting points experimentally measured for these MILs.


2015 ◽  
Vol 44 (10) ◽  
pp. 3177-3211 ◽  
Author(s):  
Maximillian J. S. Phipps ◽  
Thomas Fox ◽  
Christofer S. Tautermann ◽  
Chris-Kriton Skylaris

The partitioning of the interaction energy into chemical components such as electrostatics, polarization, and charge transfer is possible with energy decomposition analysis approaches. We review and evaluate these for biomolecular applications.


Author(s):  
Jesús Jara-Cortés ◽  
Edith Leal-Sánchez ◽  
Evelio Francisco ◽  
Jose A. Perez-Pimienta ◽  
Ángel Martín Pendás ◽  
...  

We present an implementation of the interacting quantum atoms energy decomposition scheme (IQA) with the complete active space second-order perturbation theory (CASPT2). This combination yields a real-space interpretation tool with...


2019 ◽  
Vol 807 ◽  
pp. 135-140
Author(s):  
Xi Jin Fu

Based on the first-principles, using CCSD(T) ab initio calculation method, many-body potential energy of solid argon are accurately calculated with the atomic distance R from 2.0Å to 3.6Å at T=300K, and firstly establish and discuss the face-centered cubic (fcc) atomic crystal configurations of two-, three-, and four-body terms by geometry optimization. The results shows that the total number of (Ar)2 clusters is 903, which belongs to 12 different geometric configurations, the total number of (Ar)3 clusters is 861, which belongs to 25 different geometric configurations, and the total number of (Ar)4 clusters of is 816 which belongs to 27 different geometric configurations. We find that the CCSD(T) with the aug-cc-pVQZ basis set is most accurate and practical by comprehensive consideration. The total potential energy Un reachs saturation at R>2.0Å when the only two-and three-body interaction energy are considered. When R≤2.0Å, the total potential energy Un must consider four-and higher-body interaction energy to achieve saturation. Many-body expansion potential of fcc solid argon is an exchange convergent series.


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