Dimitris Anastasakos-Paraskevopoulos, Charalampos Sarafidis, Maria Giannouri, Vasileios Alexandrakis, Ioannis Panagiotopoulos
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Martensite stabilization at RT appears to be a challenge, coexistence of martensite—austenite phases were observed and calculated for both 38–12 and 39–11 (16% and 12% austenite, respectively). Magnetization measurements versus temperature and field were recorded in the areas of interest where 1st order transitions were expected (355 K for <i>x</i> = 13 and 408 K for <i>x</i> = 14), and the magnetic entropy's changes (ΔS<sub>m</sub>) were determined [0.4 (J/kgK) for <i>x</i> = 13 and 0.3 J/(kgK) for <i>x</i> = 14; H<sub>max</sub> = 1 T]. The complex character of the magnetic properties and their dependence on Mn-Sn ratio and on the distance between Mn atoms is discussed. 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引用次数: 0
摘要
记忆形状磁性合金,尤其是 Heusler 合金,是用磁性系统取代传统冷却系统的重要材料。本研究通过电弧熔化和热处理制备了标称成分为Χ50Υ25+xΖ25-x(X = Ni; Y = Mn; Z = Sn; x = 13,14)的非化学计量 Heusler 合金。在室温(RT)和高于马氏体-奥氏体转变区的高温下,用 X 射线衍射分析了结构特性,以确定相关的晶体学参数并观察转变过程。马氏体在室温(RT)下的稳定似乎是一个挑战,在 38-12 和 39-11 (奥氏体分别为 16% 和 12%)中观察到马氏体和奥氏体相共存,并进行了计算。在预计会发生一阶转变的相关区域(x=13 时为 355 K,x=14 时为 408 K)记录了磁化率随温度和磁场变化的测量结果,并确定了磁熵变化(ΔSm)(x=13 时为 0.4 (J/kgK) ,x=14 时为 0.3 J/(kgK);Hmax=1T)。本文讨论了磁性的复杂特性及其与锰硒比和锰原子间距离的关系。本文受版权保护。本文受版权保护。
Investigation of the magnetic and structural properties in the non-stoichiometric Heusler alloy Ni50Mn25+xSn25-x; x = 13, 14
Memory shape magnetic alloys, especially Heusler alloys, are important materials in replacing conventional cooling with magnetic systems. In the present study off stoichiometric Heusler alloys with nominal composition Χ50Υ25+xΖ25-x (X = Ni; Y = Mn; Z = Sn; x = 13, 14) were prepared by arc melting followed by thermal treatment. Structural properties were analyzed with X-ray diffraction at room temperature (RT) and at elevated temperatures, above the martensite—austenite transition area, to determine the relevant crystallographic parameters and observe the transition. Martensite stabilization at RT appears to be a challenge, coexistence of martensite—austenite phases were observed and calculated for both 38–12 and 39–11 (16% and 12% austenite, respectively). Magnetization measurements versus temperature and field were recorded in the areas of interest where 1st order transitions were expected (355 K for x = 13 and 408 K for x = 14), and the magnetic entropy's changes (ΔSm) were determined [0.4 (J/kgK) for x = 13 and 0.3 J/(kgK) for x = 14; Hmax = 1 T]. The complex character of the magnetic properties and their dependence on Mn-Sn ratio and on the distance between Mn atoms is discussed. The structure and the lattice parameters were determined using an anisotropic strain broadening model; stress and strain were detected in the structure due to crystal phase coexistence.