研究论文

三方Cr5Te8 的磁结构和反常热膨胀

  • 任卫军 ,
  • 安萌 ,
  • 高飞 ,
  • 罗小华 ,
  • 李昺 ,
  • 张志东 ,
  • 王进威
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  • 1 中国科学院金属研究所 沈阳材料科学国家研究中心 沈阳 110016
    2 中国科学技术大学 材料科学与工程学院 沈阳 110016
    3 Australian Nuclear Science and Technology Organisation, New Illawarra Road, Lucas Heights, NSW 2234, Australia
任卫军,男,1970年生,研究员,博士
任卫军,wjren@imr.ac.cn,主要从事磁性材料研究

收稿日期: 2024-01-12

  修回日期: 2024-01-31

  网络出版日期: 2024-04-19

基金资助

国家重点研发计划项目(2020YFA0406002);国家自然科学基金面上项目(52071323)

Magnetic Structure and Abnormal Thermal Expansion of Trigonal Cr5Te8

  • REN Weijun ,
  • AN Meng ,
  • GAO Fei ,
  • LUO Xiaohua ,
  • LI Bing ,
  • ZHANG Zhidong ,
  • WANG Chin-Wei
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  • 1 Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China
    2 School of Materials Science and Engineering, University of Science and Technology of China, Shenyang 110016, China
    3 Australian Nuclear Science and Technology Organisation, New Illawarra Road, Lucas Heights, NSW 2234, Australia
REN Weijun, professor, Tel: (024)23971856, E-mail: wjren@imr.ac.cn

Received date: 2024-01-12

  Revised date: 2024-01-31

  Online published: 2024-04-19

Supported by

National Key Research and Development Program of China(2020YFA0406002);National Natural Science Foundation of China(52071323)

摘要

很多二元Cr-Te化合物具有NiAs结构,其中金属Cr原子出现不同程度的有序缺位。Cr5Te8有三方和单斜2种结构,本工作采用粉末X射线和中子衍射结合Rietveld全谱拟合,确定了用自助溶剂生长的三方Cr5Te8单晶具有P3¯m1晶体结构,点阵参数a = 0.3900 nm,c = 0.5986 nm。粉末中子衍射实验揭示Cr5Te8是磁矩沿c方向的共线铁磁化合物,a方向具有小的负热膨胀,c方向显示正常热膨胀。以最低温3.3 K为参考温度点,在3.3~300 K温度范围内,a方向平均热膨胀系数为-10.7 × 10-6 K-1c方向平均膨胀系数为52.4 × 10-6 K-1。[101]、[302]和[201]取向的Cr5Te8具有近零热膨胀,具备应用前景。Cr5Te8的反常热膨胀与其磁有序没有明显关联,可能与晶格中存在大量的Cr空位有关。

本文引用格式

任卫军 , 安萌 , 高飞 , 罗小华 , 李昺 , 张志东 , 王进威 . 三方Cr5Te8 的磁结构和反常热膨胀[J]. 金属学报, 2024 , 60(8) : 1150 -1154 . DOI: 10.11900/0412.1961.2024.00008

Abstract

Many binary Cr-Te compounds can be regarded as formed due to varying degrees of ordered vacancies of metal Cr atoms in Cr-Te with the NiAs structure. Among them, Cr5Te8 shows two structures: trigonal and monoclinic. This study determined that Cr5Te8 grown using the self-flux method shows a trigonal P3¯m1 crystal structure with lattice constants a = 0.3900 nm and c = 0.5986 nm, as elucidated through the Rietveld refinement of powder X-ray and neutron diffraction patterns. Neutron powder diffraction experiments reveal its collinear ferromagnetic compound, with Cr magnetic moments oriented along the c axis. In addition, it exhibits low negative thermal expansion along the a direction and normal thermal expansion along the c direction. Within the temperature range of 3.3-300 K, using the lowest temperature of 3.3 K as a reference, the average thermal expansion coefficient of Cr5Te8 is -10.7 × 10-6 and 52.4 × 10-6 K-1 in the a and c directions, respectively. Cr5Te8 crystals oriented along the [101], [302], and [201] directions show near-zero thermal expansion and thus have wide application prospects. The abnormal thermal expansion of Cr5Te8 is apparently unrelated to its magnetic order but may be related to the Cr vacancies in the crystal lattice.

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