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一级磁结构相变材料Mn0.6Fe0.4NiSi0.5Ge0.5和Ni50Mn34Co2Sn14的磁热效应与磁场的线性相关性
引用本文:张虎,邢成芬,龙克文,肖亚宁,陶坤,王利晨,龙毅.一级磁结构相变材料Mn0.6Fe0.4NiSi0.5Ge0.5和Ni50Mn34Co2Sn14的磁热效应与磁场的线性相关性[J].物理学报,2018,67(20):207501-207501.
作者姓名:张虎  邢成芬  龙克文  肖亚宁  陶坤  王利晨  龙毅
作者单位:1. 北京科技大学材料科学与工程学院, 北京 100083; 2. 佛山市程显科技有限公司, 佛山 528513; 3. 佛山市川东磁电股份有限公司, 佛山 528513; 4. 首都师范大学物理系, 北京 100048
基金项目:国家自然科学基金(批准号:51671022,51701130)、国家重点研发计划(批准号:2017YFB0702704)、北京市自然科学基金(批准号:2162022)和佛山市科技计划(批准号:2015IT100044)资助的课题.
摘    要:磁熵变(△SM)与磁场(μ0H)的相关性已在很多二级相变材料中被研究并报道,但一级相变材料的磁热效应与磁场相关性还少有报道.本文在具有一级磁结构相变的Mn0.6Fe0.4NiSi0.5Ge0.5材料中研究发现△SM与μ0H存在线性相关性,并通过麦克斯韦关系式的数值分析详细讨论了这一线性相关性的来源.同时,进一步发现在低磁场时,△SM近似正比于μ0H的平方.该线性相关性同样在一级磁结构相变Ni50Mn34Co2Sn14材料中得到了印证.但由于一级磁弹相变LaFe11.7Si1.3材料相变温度具有更强的磁场依赖性,不具有△SM的线性相关性,因此,本研究表明,当磁结构相变材料的相变温度具有弱磁场依赖性时,△SM与μ0H具有线性相关性.进而,在磁场未达到相变饱和磁场以下,利用△SM与μ0H的线性相关性可以有效推测更高磁场下的△SM.

关 键 词:磁热效应  磁熵变  磁结构相变
收稿时间:2018-05-09

Linear dependence of magnetocaloric effect on magnetic field in Mn0.6Fe0.4NiSi0.5Ge0.5 and Ni50Mn34Co2Sn14 with first-order magnetostructural transformation
Zhang Hu,Xing Cheng-Fen,Long Ke-Wen,Xiao Ya-Ning,Tao Kun,Wang Li-Chen,Long Yi.Linear dependence of magnetocaloric effect on magnetic field in Mn0.6Fe0.4NiSi0.5Ge0.5 and Ni50Mn34Co2Sn14 with first-order magnetostructural transformation[J].Acta Physica Sinica,2018,67(20):207501-207501.
Authors:Zhang Hu  Xing Cheng-Fen  Long Ke-Wen  Xiao Ya-Ning  Tao Kun  Wang Li-Chen  Long Yi
Institution:1. School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China; 2. Chengxian Technology Co. Ltd., Foshan 528513, China; 3. Chuandong Magnetic Electronic Co. Ltd., Foshan 528513, China; 4. Department of Physics, Capital Normal University, Beijing 100048, China
Abstract:The study on the field dependence of magnetocaloric effect (MCE) is considered to be of fundamental and practical importance, since it not only guides us in understanding and optimizing the MCE, but also helps us estimate the MCE for higher magnetic field which is not available in some laboratories. The magnetic field (μ0H) dependence of magnetic entropy change (△SM) has been studied extensively in many materials with second-order magnetic transition. However, the field dependence of MCE for first-order magnetic transition (FOMT) materials has not been sufficiently studied due to their complexity and diversity. In the present work, polycrystalline Mn0.6Fe0.4NiSi0.5Ge0.5, Ni50Mn34Co2Sn14, and LaFe11.7Si1.3 compounds with FOMT are prepared, and the magnetic and magnetocaloric properties are investigated systematically. In order to avoid a spurious △SM, the M-μ0H curves are measured in a loop process. The M-μ0H curves are corrected by taking into account the demagnetization effect, i.e. Hint=Hext-NdM. It is found that the -△SM follows a linear relationship -△SM=-△S0 +κμ0H with the variation of magnetic field in Mn0.6Fe0.4NiSi0.5Ge0.5 compound when μ0H > 1 T. In addition, it is also noted that the △SM is approximately proportional to the square of μ0H at low field. The origin of this linear relationship between △SM and μ0H at high field and the deviation at low field are discussed by numerically analyzing the Maxwell relation. In addition to the △SM peak value, it is found that other △SM values at different temperatures also follow the linear relation at high field by performing the same numerical analysis. Moreover, it is found that the fitted △SM curve matches the experimental data very well. This result indicates that the linear relationship between △SM and μ0H could be utilized to predict the △SM for higher magnetic field change when the field is lower than the saturation field. The applicability of this linear relationship is also verified in other systems with first-order magnetostructural transformation, such as Ni50Mn34Co2Sn14. However, it fails to describe the field dependence of △SM in LaFe11.7Si1.3, which exhibits a strong field dependence of transition temperature. Consequently, our study reveals that a linear dependence of △SM on μ0H could occur in magnetostructural transition materials, which show the field independence of transition temperature.
Keywords:magnetocaloric effect  magnetic entropy change  magnetostructural transition
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