| Autor: |
Langenberg, A., Hirsch, K., Lawicki, A., Zamudio-Bayer, V., Niemeyer, M., Chmiela, P., Langbehn, B., Terasaki, A., Issendorff, B. v., Lau, J. T. |
| Rok vydání: |
2014 |
| Předmět: |
|
| Zdroj: |
Phys. Rev. B 90, 184420 (2014) |
| Druh dokumentu: |
Working Paper |
| DOI: |
10.1103/PhysRevB.90.184420 |
| Popis: |
Spin and orbital magnetic moments of cationic iron, cobalt, and nickel clusters have been determined from x-ray magnetic circular dichroism spectroscopy. In the size regime of $n = 10 - 15$ atoms, these clusters show strong ferromagnetism with maximized spin magnetic moments of 1~$\mu_B$ per empty $3d$ state because of completely filled $3d$ majority spin bands. The only exception is $\mathrm{Fe}_{13}^+$ where an unusually low average spin magnetic moment of $0.73 \pm 0.12$~$\mu_B$ per unoccupied $3d$ state is detected; an effect, which is neither observed for $\mathrm{Co}_{13}^+$ nor $\mathrm{Ni}_{13}^+$.\@ This distinct behavior can be linked to the existence and accessibility of antiferromagnetic, paramagnetic, or nonmagnetic phases in the respective bulk phase diagrams of iron, cobalt, and nickel. Compared to the experimental data, available density functional theory calculations generally seem to underestimate the spin magnetic moments significantly. In all clusters investigated, the orbital magnetic moment is quenched to $5 - 25$\,\% of the atomic value by the reduced symmetry of the crystal field. The magnetic anisotropy energy is well below 65 $\mu$eV per atom. |
| Databáze: |
arXiv |
| Externí odkaz: |
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