The size and structural dependence of the magnetic properties of RhN clusters (9{}N{}55) are studied by using a d-electron tight-binding Hamiltonian including Coulomb interactions in the unrestricted Hartree-Fock approximation. Three main different types of cluster geometries are considered (viz., fcc, bcc, and icosahedral). In each case the equilibrium bond length R is optimized by maximizing the cohesive energy Ecoh(N). The geometries yielding the largest Ecoh(N) alternate as a function of N. These structural changes, together with the variation of R, play a crucial role in the determination of the average magnetic moment {μ}-barN of RhN. The calculated size dependence of {μ}-barN corresponding to the most stable geometries presents oscillations which are in good qualitative agreement with experiment. The magnetic properties of RhN clusters show a remarkable structural dependence which is characteristic of weak (unsaturated) itinerant ferromagnetism. The relation between the observed {μ}-barN and the cluster geometry is analyzed. The role of nonuniform geometry relaxation, sp electrons, and sp-d hybridization effects are quantified for representative examples. Perspectives of extensions of this study are also discussed.
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Villaseñor-González et al. (1997) studied this question.
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