Abstract
The definition, calculation, modelling and physical interpretation of static polarisabilities and dispersion coefficients for ions in crystals are reviewed. Ab initio calculations on clusters of ions embedded in point-charge lattices show that anions are sensitive to electrostatic and overlap interactions which reduce their polarisabilities from the free-ion values, sometimes by factors of two or more. By contrast, cations of s 2 and p 6 configuration have almost constant polarisability. Models of optical and mechanical properties of ionic solids must take into account the variation of anion polarisability with lattice parameter. A semi-quantitative treatment of dispersion coefficients can be based on the Slater-Kirkwood formula which requires only the static polarisability and one adjustable parameter (fixed by reference to the isoelectronic inert gas).