Abstract
The electronic density of states in glassy Cu−Zr has been computed by averaging the density of states of a number of clusters of atoms. The atomic positions in the clusters were chosen in such a way to reproduce the pair distribution function of the system. For each cluster the density of states was computed within the multiple-scattering theory by using Lloyd's formula. The results obtained are in fair agreement with the experimental dta. The computed density of states shows a clear split-band regime with a distance between the two main peaks comparable with the experimental results.
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