Abstract
Embedded clusters as models to study certain properties of real materials are defined as collections of atoms or ions at positions as they occur in solids and embedded in a (pseudo-) potential accounting for the short and long range, static and dynamic, influences of the rest of the material. The electronic structure is hence determined by the hamiltonian $$ H = {H^{N}}_{{cluster}} + {V_{{emb}}} $$ (1) where N indicates the number of electrons that are explicitly dealt with in the cluster chosen. The thus defined electronic problem can be treated by common ab initio or semi-empirical electronic structure methods and techniques, based on either wave functions or density functionals.
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