From Sticky-Hard-Sphere to Lennard-Jones-Type Clusters
arXiv:1801.10290 · doi:10.1103/PhysRevE.97.043309
Abstract
A relation between the set of non-isomorphic sticky hard sphere clusters and the sets of local energy minima of the -Lennard-Jones potential is established. The number of nonisomorphic stable clusters depends strongly and nontrivially on both and , and increases exponentially with increasing cluster size for . While the map from is non-injective and non-surjective, the number of Lennard-Jones structures missing from the map is relatively small for cluster sizes up to , and most of the missing structures correspond to energetically unfavourable minima even for fairly low . Furthermore, even the softest Lennard-Jones potential predicts that the coordination of 13 spheres around a central sphere is problematic (the Gregory-Newton problem). A more realistic extended Lennard-Jones potential chosen from coupled-cluster calculations for a rare gas dimer leads to a substantial increase in the number of nonisomorphic clusters, even though the potential curve is very similar to a (6,12)-Lennard-Jones potential.
10 pages
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Cited by in corpus (8)
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- Instability of the Body-Centered Cubic Lattice within the Sticky Hard Sphere and Lennard-Jones Model obtained from Exact Lattice Summations