中国物理B ›› 2023, Vol. 32 ›› Issue (6): 67504-067504.doi: 10.1088/1674-1056/ac904a

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Magnetic ordering induced magnetodielectric effect in Ho2Cu2O5 and Yb2Cu2O5

Hao Jin(金昊)1, Shuai Huang(黄帅)1,2,†, Kai-Qi Wan(万凯奇)1, Chang-Ming Zhu(朱长明)2, Hai-Ou Wang(王海欧)1, Kun-Peng Su(苏昆朋)1, and De-Xuan Huo(霍德璇)1,‡   

  1. 1 Key Laboratory of Novel Materials for Sensor of Zhejiang Province, Institute of Material Physics, Hangzhou Dianzi University, Hangzhou 310018, China;
    2 Guangxi Key Laboratory of Nuclear Physics and Nuclear Technology, Guangxi Normal University, Guilin 541004, China
  • 收稿日期:2022-05-24 修回日期:2022-09-02 接受日期:2022-09-08 出版日期:2023-05-17 发布日期:2023-05-29
  • 通讯作者: Shuai Huang, De-Xuan Huo E-mail:huangshuai@hdu.edu.cn;dxhuo@hdu.edu.cn
  • 基金资助:
    Project supported by the Young Scientists Fund of the National Natural Science Foundation of China (Grant No. 11704091), the Open Project of Guangxi Key Laboratory of Nuclear Physics and Nuclear Technology (Grant No. NLK2021-10), and the Open Project of Key Laboratory of Novel Materials for Sensor of Zhejiang Province, China (Grant No. ZJKLNMS2021010).

Magnetic ordering induced magnetodielectric effect in Ho2Cu2O5 and Yb2Cu2O5

Hao Jin(金昊)1, Shuai Huang(黄帅)1,2,†, Kai-Qi Wan(万凯奇)1, Chang-Ming Zhu(朱长明)2, Hai-Ou Wang(王海欧)1, Kun-Peng Su(苏昆朋)1, and De-Xuan Huo(霍德璇)1,‡   

  1. 1 Key Laboratory of Novel Materials for Sensor of Zhejiang Province, Institute of Material Physics, Hangzhou Dianzi University, Hangzhou 310018, China;
    2 Guangxi Key Laboratory of Nuclear Physics and Nuclear Technology, Guangxi Normal University, Guilin 541004, China
  • Received:2022-05-24 Revised:2022-09-02 Accepted:2022-09-08 Online:2023-05-17 Published:2023-05-29
  • Contact: Shuai Huang, De-Xuan Huo E-mail:huangshuai@hdu.edu.cn;dxhuo@hdu.edu.cn
  • Supported by:
    Project supported by the Young Scientists Fund of the National Natural Science Foundation of China (Grant No. 11704091), the Open Project of Guangxi Key Laboratory of Nuclear Physics and Nuclear Technology (Grant No. NLK2021-10), and the Open Project of Key Laboratory of Novel Materials for Sensor of Zhejiang Province, China (Grant No. ZJKLNMS2021010).

摘要: Materials with strongly coupled magnetic and electronic degrees of freedom provide new possibilities for practical applications. In this paper, we have investigated the structure, magnetic property, and magnetodielectric (MD) effect in Ho$_{2}$Cu$_{2}$O$_{5}$ and Yb$_{2}$Cu$_{2}$O$_{5}$ polycrystalline samples, which possess a non-centrosymmetric polar structure with space group $Pna$2$_{1}$. In Ho$_{2}$Cu$_{2}$O$_{5}$, Ho$^{3+}$ and Cu$^{2+}$ sublattices order simultaneously, exhibiting a typical paramagnetic to antiferromagnetic transition at 13.1 K. While for Yb$_{2}$Cu$_{2}$O$_{5}$, two magnetic transitions which originate from the orderings of Yb$^{3+}$ (7.8 K) and Cu$^{2+}$ (13.5 K) sublattices are observed. A magnetic field induced metamagnetic transition is obtained in these two cuprates below Néel temperature ($T_{\rm N}$). By means of dielectric measurement, distinct MD effect is demonstrated by the dielectric anomaly at $T_{\rm N}$. Meanwhile, the MD effect is found to be directly related to the metamagnetic transition. Due to the specific spin configuration and different spin evolution in the magnetic field, a positive MD effect is formed in Ho$_{2}$Cu$_{2}$O$_{5}$, and a negative one is observed in Yb$_{2}$Cu$_{2}$O$_{5}$. The spontaneous dielectric anomaly at $T_{\rm N}$ is regarded as arising from the shifts in optical phonon frequencies, and the magnetoelectric coupling is used to interpret the magnetic field induced MD effect. Moreover, an $H$-$T$ phase diagram is constructed for Ho$_{2}$Cu$_{2}$O$_{5}$ and Yb$_{2}$Cu$_{2}$O$_{5}$ based on the results of isothermal magnetic and dielectric hysteresis loops.

关键词: magnetic ordering, metamagnetic transition, magnetodielectric effect

Abstract: Materials with strongly coupled magnetic and electronic degrees of freedom provide new possibilities for practical applications. In this paper, we have investigated the structure, magnetic property, and magnetodielectric (MD) effect in Ho$_{2}$Cu$_{2}$O$_{5}$ and Yb$_{2}$Cu$_{2}$O$_{5}$ polycrystalline samples, which possess a non-centrosymmetric polar structure with space group $Pna$2$_{1}$. In Ho$_{2}$Cu$_{2}$O$_{5}$, Ho$^{3+}$ and Cu$^{2+}$ sublattices order simultaneously, exhibiting a typical paramagnetic to antiferromagnetic transition at 13.1 K. While for Yb$_{2}$Cu$_{2}$O$_{5}$, two magnetic transitions which originate from the orderings of Yb$^{3+}$ (7.8 K) and Cu$^{2+}$ (13.5 K) sublattices are observed. A magnetic field induced metamagnetic transition is obtained in these two cuprates below Néel temperature ($T_{\rm N}$). By means of dielectric measurement, distinct MD effect is demonstrated by the dielectric anomaly at $T_{\rm N}$. Meanwhile, the MD effect is found to be directly related to the metamagnetic transition. Due to the specific spin configuration and different spin evolution in the magnetic field, a positive MD effect is formed in Ho$_{2}$Cu$_{2}$O$_{5}$, and a negative one is observed in Yb$_{2}$Cu$_{2}$O$_{5}$. The spontaneous dielectric anomaly at $T_{\rm N}$ is regarded as arising from the shifts in optical phonon frequencies, and the magnetoelectric coupling is used to interpret the magnetic field induced MD effect. Moreover, an $H$-$T$ phase diagram is constructed for Ho$_{2}$Cu$_{2}$O$_{5}$ and Yb$_{2}$Cu$_{2}$O$_{5}$ based on the results of isothermal magnetic and dielectric hysteresis loops.

Key words: magnetic ordering, metamagnetic transition, magnetodielectric effect

中图分类号:  (Magnetic oxides)

  • 75.47.Lx
75.85.+t (Magnetoelectric effects, multiferroics) 77.22.-d (Dielectric properties of solids and liquids) 61.05.cp (X-ray diffraction)