Abstract
The factors that caused the Be potential to be quite different from other conventional van der Waals potentials are quantitatively delineated with relatively simple self-consistent-field calculations. By decomposing the potential into its three major components, we are able to show that the rather sudden change of slope in the potential energy curve around 3.2 Å is the result of the interplay between the hybridization and the correlation energy. It also enables us to model the interaction with a classical van der Waals potential, which provides the proper long-range behavior of the system, and a short-range attraction which mimics the effects of the hybridization.
- Received 12 November 2012
DOI:https://doi.org/10.1103/PhysRevA.88.022517
©2013 American Physical Society