马禹, 张玉洁, 张红国, 阴津华, 张宏伟, 王凤平, 王文全, 吴光恒. BiFe1-xTxO3(T=Co和Ni)的晶体结构和磁性[J]. 工程科学学报, 2010, 32(8): 1041-1044,1070. DOI: 10.13374/j.issn1001-053x.2010.08.044
引用本文: 马禹, 张玉洁, 张红国, 阴津华, 张宏伟, 王凤平, 王文全, 吴光恒. BiFe1-xTxO3(T=Co和Ni)的晶体结构和磁性[J]. 工程科学学报, 2010, 32(8): 1041-1044,1070. DOI: 10.13374/j.issn1001-053x.2010.08.044
MA Yu, ZHANG Yu-jie, ZHANG Hong-guo, YIN Jin-hua, ZHANG Hong-wei, WANG Feng-ping, WANG Wen-quan, WU Guang-heng. Magnetic properties and crystalline structure of BiFe1-xTxO3(T=Co and Ni)[J]. Chinese Journal of Engineering, 2010, 32(8): 1041-1044,1070. DOI: 10.13374/j.issn1001-053x.2010.08.044
Citation: MA Yu, ZHANG Yu-jie, ZHANG Hong-guo, YIN Jin-hua, ZHANG Hong-wei, WANG Feng-ping, WANG Wen-quan, WU Guang-heng. Magnetic properties and crystalline structure of BiFe1-xTxO3(T=Co and Ni)[J]. Chinese Journal of Engineering, 2010, 32(8): 1041-1044,1070. DOI: 10.13374/j.issn1001-053x.2010.08.044

BiFe1-xTxO3(T=Co和Ni)的晶体结构和磁性

Magnetic properties and crystalline structure of BiFe1-xTxO3(T=Co and Ni)

  • 摘要: 比较了运用固相烧结法制备的BiFe1-xCoxO3和BiFe1-xNixO3的晶体结构、饱和磁化强度和矫顽力随掺杂量的依赖关系.结果发现,强磁性的立方结构是掺杂样品磁性的主要来源.Ni掺杂样品的居里温度比Co掺杂样品高,这是由于原子间距和离子种类的不同造成了磁性离子间超交换作用的强弱变化所致.Co离子具有较强的单离子各向异性和偏离立方结构的晶格畸变,造成了Ni掺杂样品的矫顽力比Co掺杂样品低.变温磁滞回线的结果表明,BiCoO3样品的磁晶各向异性随温度降低而增大.

     

    Abstract: The doping content dependence of crystalline structures, saturation magnetization and coercivities of BiFe1-xCoxO3 was compared with that of BiFe1-xNixO3. All the samples are fabricated by solid-state sintering. It is found that ferromagnetic cubic structure in doping samples is the main source of magnetic properties. The Curie temperatures of Ni-doped samples are higher than those of Co-doped samples. The difference in Curie temperature might be due to the variation of magnetic super-exchange coupling between magnetic cations which is caused by interatomie distance and the kinds of cations. Ni-doped samples have smaller eoereivities than Codoped samples. The large coercivity results from the lattice distortion and the strong single ion anisotropy of Co cations. The results of hysteresis loops of BiCoO3 at different temperatures show that the magnetocrystalline anisotropy of BiCoO3 samples increases with decreasing temperature.

     

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