Many-body interaction and equation of state for solid krypton from ab initio calculation. (May 2015)

• Record Type: Journal Article
• Authors: Zheng, X.-R.; Fu, W.-Y.; Zhang, H.-M.; Li, Y.
• Is Part Of: Materials research innovations. Volume 19:Number 5(2015)
• Page Start: S5-782
• Page End: S5-786
• Publication Date: 2015-05
• Subjects: Materials -- Research -- Periodicals; Matériaux -- Recherche -- Périodiques; 620.1105
• DOI: 10.1179/1432891714Z.0000000001193
• Languages: German
• ISSNs: 1432-8917

Abstract

<abstract> <title> <x content-type="archive" xml:space="preserve">Abstract</x> </title> <p>Using the many-body expansion method and the double cluster with full single and double excitations plus perturbative treatment of triples [CCSD(T)] and augmented correlation consistent quadruple zeta (aug-cc-pVQZ) basis set, many-body contributions to the cohesive energy and equation of state of face-centered cubic solid krypton were accurately calculated with the atomic distance <italic>R</italic> from 2·1 to 4·0 Å at the room temperature (<italic>T = </italic>300 K) in the experimentally studied range of pressures (0–60 GPa). The results showed that many-body expansion potential of face-centered cubic solid krypton was an exchange convergent series, and the even many-body contributions to the cohesive energy were repulsive, whereas the odd many-body contributions to the cohesive energy were attractive. For the same atomic distance <italic>R</italic>, many-body potential energy would reduce when the many-body number increases. When the atomic distance <italic>R</italic>>3·4 Å, the interaction energy may be well-described by two-body potential energy. In the range of 2·4–3·4 Å, it needs to consider three-body potential energy. Below 2·4 Å, the four-body potential energy should be considered. Finally, it was studied that the isothermal compression properties of solid krypton at the pressure regions <italic>P</italic> < 60 GPa. The research results showed that the calculated and experimental results have a good consistency at the pressure ranges 0–60 GPa, and may be helpful to accurately explain the phenomenon of the experiment above 60 Gpa when the effects of four-body, five-body potential pressure are considered.</p> </abstract>