首页> 外文期刊>Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics >Structure and anisotropic compensation of Tb_(1-x)Pr_x(Fe_(0.4)Co_(0.55)B_(0.05))_(1.93) (0 = x = 1) magnetostrictive alloys
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Structure and anisotropic compensation of Tb_(1-x)Pr_x(Fe_(0.4)Co_(0.55)B_(0.05))_(1.93) (0 = x = 1) magnetostrictive alloys

机译:Tb_(1-x)Pr_x(Fe_(0.4)Co_(0.55)B_(0.05))_(1.93)(0 <= x <= 1)磁致伸缩合金的结构和各向异性补偿

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Structural, magnetic and magnetostrictive properties of Tb_(1-x)Pr_x(Fe_(0.4)Co_(0.55)B_(0.05))_(1.93) (0 < = x < = 1) alloys have been investigated. The (Tb,Pr)(Fe,Co,B)_2 compounds are found to stabilize in a cubic Laves-phase structure. The lattice parameter increases with increasing Pr content and obeys the linear Vegard's law. The spin phase diagram for the compounds is constructed to illustrate both the composition dependence of the Curie temperature (T_C) and spin reorientation temperature (T_(SR)) and the arrangement for the easy magnetization direction (EMD). It is found that T_C decreases, while T_(SR) increases as increasing Pr content. The saturation magnetization (M_s) decreases to reach a minimum when x < = 0.50, and then increases with further increasing Pr content. The composition for magnetic-moment compensation is about x_(comp) = 0.55. The magnetostriction (lambda_a) decreases with increasing Pr content when 0< = x < = 0.50, then increases with a further increasing x and exhibits a peak in the range of 0.50 < = x < = 1.0. Both the magnetization and the magnetostriction analyses show that Tb_(1-x)Pr_x(Fe_(0.4)Co_(0.55)B_(0.05))_(1.93) is an anisotropy compensation system and the compensation point is close to x= 0.80.
机译:研究了Tb_(1-x)Pr_x(Fe_(0.4)Co_(0.55)B_(0.05))_(1.93)(0 <= x <= 1)合金的结构,磁和磁致伸缩性能。发现(Tb,Pr)(Fe,Co,B)_2化合物稳定在立方Laves相结构中。晶格参数随Pr含量的增加而增加,并服从线性Vegard定律。化合物的自旋相图用于说明居里温度(T_C)和自旋重取向温度(T_(SR))的成分依赖性以及易磁化方向(EMD)的排列。发现随着Pr含量的增加,T_C降低,而T_(SR)升高。当x <= 0.50时,饱和磁化强度(M_s)减小至最小值,然后随着Pr含量的进一步增加而增大。用于磁矩补偿的成分约为x_(comp)= 0.55。当0 <= x <= 0.50时,磁致伸缩(lambda_a)随着Pr含量的增加而减小,然后随着x的进一步增加而增大,并且呈现出在0.50 <= x <= 1.0的范围内的峰值。磁化和磁致伸缩分析都表明Tb_(1-x)Pr_x(Fe_(0.4)Co_(0.55)B_(0.05))_(1.93)是各向异性补偿系统,补偿点接近x = 0.80。

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