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Co掺杂对Mn$lt;sub$gt;3$lt;/sub$gt;Sn$lt;sub$gt;1-$lt;em$gt;x$lt;/em$gt;$lt;/sub$gt;Co$lt;sub$gt;$lt;em$gt;x$lt;/em$gt;$lt;/sub$gt;C$lt;sub$gt;1.1$lt;/sub$gt;化合物的磁性质、熵变以及磁卡效应的影响
引用本文:闫君,孙莹,王聪,史再兴,邓司浩,史可文,卢会清.Co掺杂对Mn$lt;sub$gt;3$lt;/sub$gt;Sn$lt;sub$gt;1-$lt;em$gt;x$lt;/em$gt;$lt;/sub$gt;Co$lt;sub$gt;$lt;em$gt;x$lt;/em$gt;$lt;/sub$gt;C$lt;sub$gt;1.1$lt;/sub$gt;化合物的磁性质、熵变以及磁卡效应的影响[J].物理学报,2014,63(16):167502-167502.
作者姓名:闫君  孙莹  王聪  史再兴  邓司浩  史可文  卢会清
作者单位:北京航空航天大学物理系, 凝聚态物理与材料物理研究中心, 北京 100191
摘    要:利用固态反应法制备了Mn3Sn1-xCoxC1.1 (x=0.05,0.1,0.2) 系列化合物,研究了Co掺杂对其磁性质、相变、熵变的影响. 随着Co掺杂量的增加,样品的居里温度由283 K先降到212 K (Mn3Sn0.9Co0.1C1.1) 后又升到332 K (Mn3Sn0.2Co0.8C1.1),相变类型由一级相变逐渐转变为二级相变. 增大Co的掺杂量,Mn3Sn1-xCoxC1.1化合物的熵变峰值逐渐减小,磁熵变温区由9 K展宽到300 K. 当Co掺杂量为0.2时,相对制冷量达到最高,为103 J/kg (磁场强度为1.6 MA/m). 由于室温附近良好的磁致冷效应,该类材料在磁制冷领域可能具有重要的应用前景. 关键词: 磁性质 相变 磁卡效应 相对制冷量

关 键 词:磁性质  相变  磁卡效应  相对制冷量
收稿时间:2014-03-25

Effects of Co doping on the magnetic properties,entropy change,and magnetocaloric effect in Mn3Sn1-xCoxC1.1compounds
Yan Jun,Sun Ying,Wang Cong,Shi Zai-Xing,Deng Si-Hao,Shi Ke-Wen,Lu Hui-Qing.Effects of Co doping on the magnetic properties,entropy change,and magnetocaloric effect in Mn3Sn1-xCoxC1.1compounds[J].Acta Physica Sinica,2014,63(16):167502-167502.
Authors:Yan Jun  Sun Ying  Wang Cong  Shi Zai-Xing  Deng Si-Hao  Shi Ke-Wen  Lu Hui-Qing
Abstract:The Mn3Sn1-xCoxC1.1 compounds are synthesized by a solid-state reaction method. The effects of Co doping on the magnetic properties, phase transition and entropy change are investigated in Mn3Sn1-xCoxC1.1 compounds. The Curie temperature first decreases from 283 K to 212 K (Mn3Sn0.9Co0.1C1.1) with increasing the Co concentration, and then increases to 332 K (Mn3Sn0.2Co0.8C1.1) with further increasing the Co concentration in Mn3Sn1-xCoxC1.1. The first-order transition of Mn3Sn1-xCoxC1.1 gradually changes into the second-order transition, in the mean time, the entropy change decreases and the phase transition region broadens from 9 K to 300 K with increasing the Co content. Both the magnetic entropy change and broadening the transition temperature span can influence the relative cooling power R. Finally we obtain the large R=103 J/kg (H=1.6 MA/m) in Mn3Sn0.8Co0.2C1.1, which could be used as the room-temperature magnetic refrigerant materials.
Keywords: magnetic properties phase transition magnetocaloric effect relative cooling power
Keywords:magnetic properties  phase transition  magnetocaloric effect  relative cooling power
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