Electronic structure and magnetism of the diluted magnetic semiconductor Fe-doped ZnO nano-particles
T. Kataoka, M. Kobayashi, Y. Sakamoto, G. S. Song, A. Fujimori, F.-H., Chang, H.-J. Lin, D. J. Huang, C. T. Chen, T. Ohkochi, Y. Takeda, T. Okane,, Y. Saitoh, H. Yamagami, A. Tanaka, S. K. Mandal, T. K. Nath, D. Karmakar and, I. Dasgupta

TL;DR
This study investigates the electronic structure and origin of room-temperature ferromagnetism in Fe-doped ZnO nanoparticles using advanced spectroscopic techniques, revealing Fe ions mainly in the Fe$^{3+}$ state and antiferromagnetic coupling as the ferromagnetism source.
Contribution
It provides detailed spectroscopic analysis showing Fe ions are mostly Fe$^{3+}$ and identifies antiferromagnetic coupling as the origin of ferromagnetism in Fe-doped ZnO nanoparticles.
Findings
Fe ions are predominantly Fe$^{3+}$ with some Fe$^{2+}$.
Fe$^{3+}$ ions are mainly at the surface region.
Room temperature ferromagnetism arises from antiferromagnetic coupling.
Abstract
We have studied the electronic structure of ZnFeO nano-particles, which have been reported to show ferromagnetism at room temperature, by x-ray photoemission spectroscopy (XPS), resonant photoemission spectroscopy (RPES), x-ray absorption spectroscopy (XAS) and x-ray magnetic circular dichroism (XMCD). From the experimental and cluster-model calculation results, we find that Fe atoms are predominantly in the Fe ionic state with mixture of a small amount of Fe and that Fe ions are dominant in the surface region of the nano-particles. It is shown that the room temperature ferromagnetism in the ZnFeO nano-particles is primarily originated from the antiferromagnetic coupling between unequal amounts of Fe ions occupying two sets of nonequivalent positions in the region of the XMCD probing depth of 2-3 nm.
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