Abstract

Theoretical studies on M13_{13} (M = Fe, Co, Ni) and M13_{13}Ptn_n (for nn = 3, 4, 5, 20) clusters including the spin-orbit coupling are done using density functional theory. The magnetic anisotropy energy (MAE) along with the spin and orbital moments are calculated for M13_{13} icosahedral clusters. The angle-dependent energy differences are modelled using an extended classical Heisenberg model with local anisotropies. From our studies, the MAE for Jahn-Teller distorted Fe13_{13}, Mackay distorted Fe13_{13} and nearly undistorted Co13_{13} clusters are found to be 322, 60 and 5 μμeV/atom, respectively, and are large relative to the corresponding bulk values, (which are 1.4 and 1.3 μμeV/atom for bcc Fe and fcc Co, respectively.) However, for Ni13_{13} (which practically does not show relaxation tendencies), the calculated value of MAE is found to be 0.64 μμeV/atom, which is approximately four times smaller compared to the bulk fcc Ni (2.7 μμeV/atom). In addition, MAE of the capped cluster (Fe13_{13}Pt4_4) is enhanced compared to the uncapped Jahn-Teller distorted Fe13_{13} cluster.

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