Abstract
A microscopic analysis of the differences in Gibbs free energy between covalent, ionic, and metallic forms of ANB8N compounds is described. The analysis explains the success of the spectroscopic theory of chemical bonds in predicting the covalent-ionic transition at zero pressure as a function of A and B. It also suggests that bond charge may play the role of a microscopic order parameter which determines the magnitude of the differences in energy between ionic and covalent structures at zero pressure and temperature.