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Phys. Rev. B 75, 195215 (2007) [7 pages]

Effect of Co and O defects on the magnetism in Co-doped ZnO: Experiment and theory

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G. S. Chang1,*, E. Z. Kurmaev2, D. W. Boukhvalov3, L. D. Finkelstein2, S. Colis4, T. M. Pedersen1, A. Moewes1, and A. Dinia4
1Department of Physics and Engineering Physics, University of Saskatchewan, 116 Science Place, Saskatoon, SK, Canada S7N 5E2
2Institute of Metal Physics, Russian Academy of Sciences–Ural Division, 620041 Yekaterinburg, Russia
3Institute for Molecules and Materials, Radboud University, NL-6525 ED Nijmegen, The Netherlands
4IPCMS CNRS-UMR 7504, ULP-ECPM, 23 Rue du Loess, F-67034 Strasbourg, France

Received 9 November 2006; revised 12 February 2007; published 29 May 2007

The electronic structure of Zn1−xCoxO (x=0.02, 0.06, and 0.10) diluted magnetic semiconductors is investigated using soft x-ray emission spectroscopy and first-principles calculations. X-ray absorption and emission measurements reveal that most Co dopants are incorporated at the Zn sites and that free charge carriers are absent over a wide range of Co concentrations. The excess Co interstitials appear in the samples with high Co concentration (10 at. %) but are isolated without any direct exchange interaction with substitutional Co atoms. The lack of free charge carriers and the direct Co-Co interactions is responsible for the absence of ferromagnetism in the samples. First-principles calculations suggest that the exchange interaction between substitutional Co atoms induces only an antiferromagnetic coupling, and strong ferromagnetism in Co-doped ZnO requires not only free charge carriers but also the Co interstitials directly interacting with substitutional Co atoms.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.75.195215
DOI:
10.1103/PhysRevB.75.195215
PACS:
78.70.En, 75.50.Pp, 71.20.Nr, 75.30.Hx

*Corresponding author. E-mail address: gapsoo.chang@usask.ca