Volume 242, Issue 10 pp. 2129-2137
Original Paper

Crystal structure and magnetic properties of mixed compounds Nd1–xRxCo3 (R = Gd, Tb)

Z. W. Ouyang

Z. W. Ouyang

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, PR China

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G. H. RaoW. F. Liu

W. F. Liu

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, PR China

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G. Y. Liu

G. Y. Liu

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, PR China

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X. M. Feng

X. M. Feng

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, PR China

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J. K. Liang

J. K. Liang

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, PR China

International Center for Materials Physics, Academia Sinica, Shenyang 110015, PR China

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First published: 04 July 2005
Citations: 2

Abstract

The crystal structure and magnetic properties of Nd1–xRxCo3 (R = Gd, Tb) have been investigated by means of X-ray powder diffraction and magnetic measurements. Spin reorientation and magnetization compensation are observed in both systems. The saturation magnetization MS of Nd1–xTbxCo3 exhibits an anomaly at a critical concentration xc ≈ 0.55, whereas no such an anomaly is observed for Nd1–xGdxCo3. These observations could be understood by considering the difference of the anisotropy between Tb3+ and Gd3+ ions. The type of magnetocrystalline anisotropy of the compounds is derived based on X-ray diffraction patterns of the field-aligned samples. For Nd1–xTbxCo3, the anisotropy near xc is weak with an undefined easy magnetization direction. On the Nd-rich side, the anisotropy exhibits a strong temperature dependence. (© 2005 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

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