Abstract

The absorption spectra of transition-metal-doped alkali halide systems are distinguished by characteristic features identified with transitions between electron states localized on the impurity ion. The theoretical description of these features depends on a realistic treatment of the host crystal electronic structure, as well as on the treatment of the impurity ion. The success of recent calculations using the self-interaction-corrected local-spin-density (SIC-LSD) form of density-functional theory in determining the band structure of alkali halide crystals makes SIC-LSD a good candidate for use in the impurity problem. In this work SIC-LSD is applied to the NaCl:${\mathrm{Cu}}^{+}$ impurity system, using an embedded-cluster technique explicitly including seven near-neighbor shells of the host crystal ions around the ${\mathrm{Cu}}^{+}$ site, allowing a full characterization of the low-lying impurity excited states. The calculated values for the fundamental 3d\ensuremath{\rightarrow}4s and 3d\ensuremath{\rightarrow}4p impurity-ion transitions are in close agreement with corresponding features of the NaCl:${\mathrm{Cu}}^{+}$ absorption spectrum. We compare and contrast our SIC-LSD results with those of other recent calculations for NaCl:${\mathrm{Cu}}^{+}$.

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