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Absence of ferromagnetism in bulk polycrystalline<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mi>Zn</mml:mi><mml:mn>0.9</mml:mn></mml:msub><mml:msub><mml:mi>Co</mml:mi><mml:mn>0.1</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math>

Sheng YinLaboratory of New-Structured Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, People's Republic of ChinaMingxiang XuNew Materials Group, Superconducting Materials Center, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, JapanLin YangLaboratory of New-Structured Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, People's Republic of ChinaJ. F. LiuLaboratory of New-Structured Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, People's Republic of ChinaH. RösnerHorst HahnH. GleiterInstitute for Nanotechnology, Forschungszentrum Karlsruhe, P.O. Box 3640, 76021 Karlsruhe, GermanyDieter SchildInstitute for Nuclear Waste Disposal, Forschungszentrum Karlsruhe, P.O. Box 3640, 76021 Karlsruhe, GermanySpencer DoyleTao LiuInstitute of High Energy Physics, Chinese Academy of Sciences, Beijing 100039, People's Republic of ChinaT. HuInstitute of High Energy Physics, Chinese Academy of Sciences, Beijing 100039, People's Republic of ChinaE. Takayama‐MuromachiNew Materials Group, Superconducting Materials Center, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, JapanJie JiangLaboratory of New-Structured Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, People's Republic of China
2006lv
ABI

Аннотация

The atomic structure and the magnetic properties of 5 and $10\phantom{\rule{0.3em}{0ex}}\mathrm{at}.\phantom{\rule{0.2em}{0ex}}%$ Co-doped $\mathrm{ZnO}$ samples prepared by a high-pressure and high-temperature method have been investigated by various techniques, including x-ray diffraction with Rietveld refinements, scanning electron microscopy, high-resolution transmission electron microscopy, nanometer-sized element mapping, x-ray photoelectron spectroscopy, near-edge x-ray absorption fine structure, and extended x-ray absorption fine structure and magnetization measurements. It is found that Co ions with a valence of $2+$ substitute Zn ions in the wurtzite $\mathrm{ZnO}$ structure. No metallic or oxidic Co-rich clusters were detected in the samples. If ${\mathrm{Co}}^{2+}$ ions substitute ${\mathrm{Zn}}^{2+}$ ions, no intrinsic ferromagnetism is observed in $\mathrm{ZnO}$ at doping levels up to $10\phantom{\rule{0.3em}{0ex}}\mathrm{at}.\phantom{\rule{0.2em}{0ex}}%$ Co even down to $5\phantom{\rule{0.3em}{0ex}}\mathrm{K}$. A paramagnetic behavior with partially antiferromagnetic interactions is observed. Thus, in bulk Co-doped $\mathrm{ZnO}$ system any observation of ferromagnetism is probably due to small clusters of second phase materials. However, in thin films the situation might be more complex, since other extrinsic influences, such as strain or proximity effects, may modify the electronic and magnetic properties.

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