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Er3(Fe,Co, M)29化合物(M=Cr,V, Ti,Mn, Ga,Nb)的结构与磁性
引用本文:罗鸿志,贾 琳,李养贤,孟凡斌,申 江,陈难先,吴光恒,杨伏明.Er3(Fe,Co, M)29化合物(M=Cr,V, Ti,Mn, Ga,Nb)的结构与磁性[J].物理学报,2005,54(11):5246-5250.
作者姓名:罗鸿志  贾 琳  李养贤  孟凡斌  申 江  陈难先  吴光恒  杨伏明
作者单位:(1)北京科技大学应用物理研究所,北京 100083; (2)河北工业大学材料学院,天津 300130; (3)中国科学院物理研究所北京凝聚态物理国家实验室,北京 100080; (4)中国科学院物理研究所北京凝聚态物理国家实验室,北京 100080;北京科技大学应用物理研究所,北京 100083; (5)中国科学院物理研究所北京凝聚态物理国家实验室,北京 100080;河北工业大学材料学院,天津 300130
基金项目:国家自然科学基金(批准号:TG2000067106)资助的课题.
摘    要:合成了ErFe29-x-yCoxMy化合物(M=Cr, V, Ti, Mn, Ga, Nb )并用x射线衍射和磁测量等手段研究了它们的结构和磁性. 发现Fe基Er(Fe,M)29化合物结晶成哑铃对Fe-Fe无序替代的Th2Ni17型结构(P63/mmc空间群)而不能形成Nd3(Fe,Ti)29型结构,因此其化学式也可以用Er2-n(Fe,M)17+2n (n=0.2)表示. 当ErFe29化合物中部分Fe原子被M原子所取代时,其居里温度均有一定程度的提高. 所有Er(Fe,M)29化合物在室温均为易面型各向异性. 当Er(Fe,M)29 (M=Cr, V)中的部分Fe原子被Co原子取代且Co原子数与Fe原子数达到一定比值时,得到一个单斜结构的新相. 磁测量表明ErFe19.5Co6V3.5在室温可能为单轴各向异性,在162K出现自旋重取向,其各向异性由易轴型变为易面型. 在5K下于难磁化方向磁化时观察到一个一级磁化过程(FOMP). 关键词: 稀土金属间化合物 晶体结构 磁晶各向异性

关 键 词:稀土金属间化合物  晶体结构  磁晶各向异性
文章编号:1000-3290/2005/54(11)/5246-05
收稿时间:01 20 2005 12:00AM
修稿时间:2005-01-202005-03-31

Structure and magnetic properties of Er3(Fe, Co, M)29 compounds (M=Cr, V, Ti, Mn, Ga, Nb)
Luo Hong-Zhi,Jia Lin,Li Yang-Xian,Meng Fan-Bin,Shen Jiang,Chen Nan-Xian,Wu Guang-Heng and Yang Fu-Ming.Structure and magnetic properties of Er3(Fe, Co, M)29 compounds (M=Cr, V, Ti, Mn, Ga, Nb)[J].Acta Physica Sinica,2005,54(11):5246-5250.
Authors:Luo Hong-Zhi  Jia Lin  Li Yang-Xian  Meng Fan-Bin  Shen Jiang  Chen Nan-Xian  Wu Guang-Heng and Yang Fu-Ming
Institution:1.Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, China; 2.School of Material Science and Engineering, Hebei University of Technology, Tianjin 300130, China; 3.Institute of Physics, Beijing University of Science and Technology, Beijing 100083, China
Abstract:A series of Er_3(Fe, Co, M)_ 29 (M=Cr, V, Ti, Mn, Ga, Nb) compounds has been synthesized and their structure and magnetic properties have been investigates by means of x-ray diffraction and magnetic measurements. It is found that the Fe-based Er_3(Fe,M)_ 29 compounds crystallize in the Th_2Ni_ 17-type structure with disordered substitution of the dumbbell Fe-Fe, instead of Nd_3(Fe,Ti)_ 29-type structure, so its chemical formula can also be expressed as Er_ 2-n(Fe,M)_ 17 2n (n=0.2). Substitution of M for Fe in the Er_3Fe_ 29 compound leads to an increase in the Curie temperature. With the substitution of Co for Fe in the Er_3(Fe,M)_ 29 (M=Cr, V) compounds, a new phase was found which crystallizes in monoclinic symmetry. The anisotropy of the Er_3Fe_ 19.5Co_6V_ 3.5 compound at room temperature is of easy-axis type and a spin reorientation transition from the easy-axis type to the easy-plane type anisotropy occurs when temperature decreases to 162K. A first order magnetization process (FOMP) was observed in the HMD magnetization curve of Er_3Fe_ 19.5Co_6V_ 3.5 at 5K, the critical field of the FOMP was derived to be 3.8T.
Keywords:rare earth transition metal intermetallic compounds  crystal structure  magnetocrystalline anisotropy
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