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Magnetic properties of LnMnO(3) (Ln=Ho, Er,Tm,Yb, and Lu)

机译:LnMnO(3)的磁性(Ln = Ho,Er,Tm,Yb和Lu)

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Magnetic data are presented for LnMnO(3) (Ln = Ho, Er, Tm, Yb, and Lu) having the hexagonal crystal structure of P6(3)cm. DC magnetization measurements show that magnetic order is not clearly observed for Ln = Ho-Yb, while an antiferromagnetic transition of the Mn3+ moments is found at similar to90 K for LuMnO3, where the Lu3+ ion has no 4f localized moment. This is ascribed to both the paramagnetism of Ln(3+) an the suppression of magnetization in the Mn3+ sublattices arising from strong antiferromagnetic interactions between Mn Deviation from the Curie-Weiss law at low temperatures indicates the onset of antiferromagnetism. Some magnetization data of Ca-substituted compounds, Ln(0.5)Ca(0.5)MnO(3), which have the different crystal structure of orthorhombic Pnma, are also discussed briefly. (C) 2002 Elsevier Science (USA). [References: 21]
机译:给出了具有P6(3)cm六方晶体结构的LnMnO(3)(Ln = Ho,Er,Tm,Yb和Lu)的磁数据。直流磁化测量表明,对于Ln = Ho-Yb,没有清楚地观察到磁序,而对于LuMnO3,发现Mn3 +矩的反铁磁跃迁类似于90 K,其中Lu3 +离子没有4f局部矩。这既可以归因于Ln(3+)的顺磁性,又可以抑制Mn之间的强反铁磁相互作用引起的Mn3 +子晶格中的磁化,这是由于低温下居里-魏斯定律的偏离表明了反铁磁性的开始。还简要讨论了Ca-取代的化合物Ln(0.5)Ca(0.5)MnO(3)的磁化数据,这些化合物具有正交晶的Pnma的不同晶体结构。 (C)2002 Elsevier Science(美国)。 [参考:21]

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