Comparison of ab initioMODPOT interaction energy components against large basis set MBPT (4) calculations for nitromethane dimer

1987 ◽  
Vol 32 (S21) ◽  
pp. 645-660 ◽  
Author(s):  
W. A. Sokalski ◽  
P. C. Hariharan ◽  
Joyce J. Kaufman
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.


2008 ◽  
Vol 29 (11) ◽  
pp. 1725-1732 ◽  
Author(s):  
Laban Bondesson ◽  
Elias Rudberg ◽  
Yi Luo ◽  
Paweł Sałek

1986 ◽  
Vol 84 (9) ◽  
pp. 5077-5080 ◽  
Author(s):  
F. J. Olivares del Valle ◽  
S. Tolosa ◽  
J. J. Esperilla ◽  
E. A. Ojalvo ◽  
A. Requena

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