{"title":"Structure, magnetization and magnetoelectric properties of double perovskite Y2CoMnO6","authors":"Gaoshang Gong, Xiaoying Chen, Yanxin Gao, Minghao Wang, Yongqiang Wang, Yuling Su","doi":"10.1016/j.jallcom.2025.179842","DOIUrl":null,"url":null,"abstract":"The multiferroic property of double perovskite R<sub>2</sub>CoMnO<sub>6</sub> (R=Rare Earth) compounds remains controversial. To clarify this problem, Y<sub>2</sub>CoMnO<sub>6</sub> was synthesized. Its structure, magnetization and magnetoelectric properties were studied. The lattice parameters of Y<sub>2</sub>CoMnO<sub>6</sub> are a = 5.2362(3) Å, b = 5.5900(3) Å and c = 7.4750(4) Å, respectively. The monoclinic angle is β = 89.8(1)°. They approach to the values of Lu<sub>2</sub>CoMnO<sub>6</sub>. The ordered Co<sup>2+</sup>/Mn<sup>4+</sup> cations favor a long-range ferromagnetic coupling, with some glassy phase exists due to the partial disordered Co<sup>2+</sup>/Mn<sup>4+</sup>. The absence of anomaly in dielectric constant and dielectric loss curves around the magnetic transition temperature suggests that Y<sub>2</sub>CoMnO<sub>6</sub> is a typical paraelectric material. The observed pyroelectric current and polarization are thus attributed to the domain wall effect. I.e., from paramagnetic state to ferromagnetic state, the Co<sup>2+</sup>-Mn<sup>4+</sup> bonds and Mn<sup>4+</sup>-Co<sup>2+</sup> bonds carry opposite electric dipole. In electric field, the reverse of the domain walls can establish a net electric polarization. Finally, a detectable pyroelectric current is resulted. Both the magnetic domain and freezing spin play a role in the magnetodielectric coupling of Y<sub>2</sub>CoMnO<sub>6</sub>. The reverse of magnetic domain tends to decrease the dielectric permittivity, while the flip of the freezing glassy component has a positive contribution to the capacitance.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"59 1","pages":""},"PeriodicalIF":5.8000,"publicationDate":"2025-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Alloys and Compounds","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jallcom.2025.179842","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
The multiferroic property of double perovskite R2CoMnO6 (R=Rare Earth) compounds remains controversial. To clarify this problem, Y2CoMnO6 was synthesized. Its structure, magnetization and magnetoelectric properties were studied. The lattice parameters of Y2CoMnO6 are a = 5.2362(3) Å, b = 5.5900(3) Å and c = 7.4750(4) Å, respectively. The monoclinic angle is β = 89.8(1)°. They approach to the values of Lu2CoMnO6. The ordered Co2+/Mn4+ cations favor a long-range ferromagnetic coupling, with some glassy phase exists due to the partial disordered Co2+/Mn4+. The absence of anomaly in dielectric constant and dielectric loss curves around the magnetic transition temperature suggests that Y2CoMnO6 is a typical paraelectric material. The observed pyroelectric current and polarization are thus attributed to the domain wall effect. I.e., from paramagnetic state to ferromagnetic state, the Co2+-Mn4+ bonds and Mn4+-Co2+ bonds carry opposite electric dipole. In electric field, the reverse of the domain walls can establish a net electric polarization. Finally, a detectable pyroelectric current is resulted. Both the magnetic domain and freezing spin play a role in the magnetodielectric coupling of Y2CoMnO6. The reverse of magnetic domain tends to decrease the dielectric permittivity, while the flip of the freezing glassy component has a positive contribution to the capacitance.
期刊介绍:
The Journal of Alloys and Compounds is intended to serve as an international medium for the publication of work on solid materials comprising compounds as well as alloys. Its great strength lies in the diversity of discipline which it encompasses, drawing together results from materials science, solid-state chemistry and physics.