Type I FA (Rb +, Cs +) and II FA (Li +, Na +) tunable laser activities and donor-acceptor properties of O and O − at KCl (001) surface: first principle calculations

Abstract

Type I F A (Rb +, Cs +) and II F A (Li +, Na +) tunable laser activities, adsorptivity and donor-acceptor properties of O and O − adsorbates at the flat surface of KCl crystal were investigated using an embedded cluster model and ab initio methods of molecular electronic structure calculations. Ion clusters were embedded in a simulated Coulomb field that closely approximates the Madelung field of the host surface, and the nearest neighbor ions to the defect site were allowed to relax to equilibrium. Based on the calculated Stokes shifted optical transition bands, F A tunable laser activities were found to be inversely proportional to the size of the dopant cation (Li +, Na +, Rb +, Cs +) relative to the host cation (K +). This relation was explained in terms of the axial perturbation of the impurity cation. The probability of orientational bleaching attributed to the RES saddle point ion configuration along the 〈110〉 axis was found to be inversely proportional to the size of the dopant cation, with activation energy barriers of ca. 0.44–3.34 eV. Surface relaxation energies of type II F A centers were more important than those of type I F A centers. In terms of defect formation energies, the products of type II F A center imperfection were more stable than those of type I F A. The difference between F or F A band energies and exciton bands depended almost exclusively on the size of the positive ion species. As far as the adsorptivity of O and O − is concerned, the results confirm that surface imperfection enhances the adsorption energies by ca. 4.38–16.37 eV. O and O − penetrate through the defect-containing surface. The energy gap between the adsorbate and the defect containing surface and the donor-acceptor property of adsorbate play the dominant role in the course of adsorbate substrate interactions and the results were explained in terms of electrostatic potential curves and Mulliken population analysis.