Clusters / Molecular Structure / SpectroscopyThe a&-initio configuration interaction study of excited states of small alkali metal clusters accounts fully for the spectroscopic patterns recorded by depletion or/and femtosecond spectroscopy and permits geometrical assignment. Specific structural and electronic properties responsible for excitations in small Ia/IIa clusters allow for the interpretation of theoretical and experimental findings in the framework of a molecular many-electron description. Similarities and differences between optical response properties of Li, and Nan clusters are discussed. The influence of the position of a divalent heteroatom in the geometrical structures of Na,Mg clusters on spectroscopical patterns will be presented. The reliability of simplified methods such as random phase approximation (RPA) and multiconfigurational linear response method (MCLR) for optically allowed transitions in metal clusters has been examined.
IntroductionThe nature of excitations in simple metal clusters which is responsible for spectroscopic patterns characterized by relatively small number of intense and a large number of weak optically allowed transitions has recently been a subject of intense experimental [l -121 and theoretical (cf. [13] and references therein) investigations. It is of particular interest to gain an understanding of the physical phenomena responsible for the characteristic spectroscopic patterns as functions of the cluster size, its shape and chemical composition. In alkali metal clusters the bonding is characterized by multicenter delocalized bonds reflecting the delocalized nature of s1 electrons rather than by directioned two center bonds which are characteristic for the localized bonding. In addition, very small Li and Na clusters do not assume highly symmetrical shapes due to the Jahn-Teller deformation. If the number of valence electrons is not sufficient to fill up the degenerate one electron levels of highly symmetrical structures, which are three-dimensional, deformations lead to the most stable planar structures. Therefore, tetramers with four valence electrons assume rhombic geometries and the octamers with eight valence electrons have three-dimensional compact symmetrical ( Td) geometries built from tetrahedral subunits [13,14]. This structural information has recently been confirmed by a comparison of ab-initio configuration interaction (CI) predictions [13,15 -231 with the depletion spectra [3 -8,11,22,23]. In this contribution we address the following issues: