4.7 Article

Dielectric properties and magnetoelectric coupling in polar magnet (Fe, Zn)2Mo3O8

Journal

CERAMICS INTERNATIONAL
Volume 48, Issue 17, Pages 24326-24331

Publisher

ELSEVIER SCI LTD
DOI: 10.1016/j.ceramint.2022.04.274

Keywords

Fe2Mo3O8; Magnetoelectric coupling; Multiferroics; Single crystals

Funding

  1. Science and Technology Program of Guangzhou [2019050001]
  2. GDAS' Project of Science and Technology Development [2021GDASYL-20210103075, 2021GDASYL-20210103074]
  3. China Postdoctoral Science Foundation [2021M690748, 2021TQ0080]
  4. Shenzhen Peacock Plan
  5. Harbin institute of technology, Shenzhen
  6. Guangdong Province through Characteristic In-novation Project [2021KTSCX364]

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The study investigated the magnetodielectric and magnetoelectric effects of (Fe1-xZnx)(2)Mo3O8 single crystals, revealing sharp MD effect in FMO and modulated magnetization M by electric field E. The ME response to Zn2+ dopants showed different behavior at two temperature ranges in (Fe0.95Zn0.05)(2)Mo3O8.
A complete understanding of magnetoelectric (ME) coupling in polar magnet Fe2Mo3O8 (FMO) remains elusive. Here, we report the magnetodielectric (MD) and ME effects of (Fe1-xZnx)(2)Mo3O8 (x = 0, 0.05) single crystals. The observation of MD effect in FMO shows a sharp peak once T is below T-N due to the metamagnetic transition, which is converted into an obvious step upon cooling. Meanwhile, the change of magnetization M modulated by electric field E is striking at the dielectric constant peak/step. In (Fe0.95Zn0.05)(2)Mo3O8, however, the sharp peak at just below T-N is intact, while the step at much lower T-N is highly damaged. The ME response to 5% Zn2+ dopants at the two T-ranges shows different behavior. Combining with spin wave theory, it is possible to speculate that the inverse Dzyaloshinskii-Moriya interaction might play a dominant role in the ME nature at just below T-N, which is different from that at much lower T-N.

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