Coercive Force of Co–CoO Thin Films
A Co-CoO system was studied to obtain high coercive materials. Co-CoO thin films were sputtered at various O gas flow rates by dual ion-beam sputtering. The Co was deposited onto glass substrates at RT and 650 K by Ar ion-beam sputtering and simultaneously oxidized by O gas from an assist ion gun. A...
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Published in | Japanese Journal of Applied Physics Vol. 41; no. Part 1, No. 10; pp. 5982 - 5985 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
2002
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Online Access | Get full text |
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Summary: | A Co-CoO system was studied to obtain high coercive materials. Co-CoO thin films were sputtered at various O gas flow rates by dual ion-beam sputtering. The Co was deposited onto glass substrates at RT and 650 K by Ar ion-beam sputtering and simultaneously oxidized by O gas from an assist ion gun. As the O gas flow rate increases, there appear Co, the Co-CoO mixed phase, CoO, and Co2O3 in a stepwise manner. The coercive force increases sharply in the Co-CoO mixed phase region. However, the maximum coercive force at RT is small, about 600 Oe. At low temperatures, the addition of the CoO phase to Co causes a significant increase of the coercive force. The perpendicular coercive force of the Co-CoO film is larger than the in-plane coercive force. The perpendicular coercive force is about 17000 Oe at about 10 K. This is due to the magnetic anisotropy of the antiferromagnetic microcrystalline CoO below the Neel temperature of about 220 K. The CoO (111) plane is preferably oriented and the spin axis of CoO stands against the plane, which leads to a strong perpendicular magnetic anisotropy. There is a possibility that the coexistence of the ferromagnetic phase and the antiferromagnetic phase increases the coercive force. 5 refs. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0021-4922 1347-4065 |
DOI: | 10.1143/JJAP.41.5982 |