You are currently viewing a new version of our website. To view the old version click .
Proceedings
  • Abstract
  • Open Access

22 November 2023

Crystal and Magnetic Structure Transitions in Doped Lu- and Fe-Based Perovskite Oxides †

,
,
,
,
,
,
,
and
1
Institute of Chemistry, Vilnius University, 01513 Vilnius, Lithuania
2
Department of Organic Chemistry, Center for Physical Sciences and Technology (FTMC), 10257 Vilnius, Lithuania
3
Namangan Engineering-Construction Institute, Dustlik Avenue 4, Namangan 160100, Uzbekistan
4
IPCMS (UMR 7504 CNRS), University of Strasbourg, 67000 Strasbourg, France
This article belongs to the Proceedings International Conference EcoBalt 2023 "Chemicals & Environment"
The possibility of controlling physical properties via chemical doping is particularly important when considering the formation of both electrical and magnetic orderings in the same compounds, which are commonly referred as multiferroics [1]. However, for the most part, due to the conflicting nature of these properties, the coupling between the electrical and magnetic properties is relatively weak. Recently, a new class of hexagonal rare earth ferrite perovskite compounds has been found to exhibit multiferroic ordering, with a mechanism and structure similar to that of hexagonal manganites, making them a new avenue for potential research. This new family of room temperature multiferroic compounds is based on LuFeO3 with a hexagonal structure (space group P63cm). It has been discovered that LuFeO3 in its hexagonal state has both ferroelectric and weak ferromagnetic orderings [2,3]. As such, in this work, we adapted an ethylene glycol based sol-gel synthesis procedure for the preparation of bulk Sc doped hexagonal lutetium ferrite powders. The crystal structure was investigated using XRD and Raman spectroscopy at room temperature. The temperature-driven crystal structure transitions were analyzed by means of in situ high-temperature XRD while the magnetic transitions were investigated by means of low-temperature magnetization measurements. The obtained results revealed that at room temperature, the polar hexagonal phase can be stabilized in a quite narrow doping range that depends on the sintering temperature of the samples [4]. Additionally, samples with a higher Sc doping content showed a lower phase transition temperature from ferroelectric to paraelectric phases. While Sc itself is not magnetic, the Sc doping caused substantial changes to the magnetization of the samples as well. Overall, the results indicate that LuFeO3 can be successfully synthesized by means of the ethylene glycol based sol-gel procedure. The desired phase composition, magnetic and electric properties can be optimized by means of the doping content and the sintering temperature.

Author Contributions

Conceptualization, A.K., R.S. and D.K.; methodology, A.P. and S.-W.C.; formal analysis, A.P., D.K., G.R. and G.N.; investigation, A.P., G.R., S.-W.C. and G.N.; resources, P.R., A.K. and T.C.-K.Y.; data curation, R.S. and P.R.; writing—original draft preparation, G.R., A.P. and D.K.; writing—review and editing, D.K. and A.P.; visualization, A.P, S.-W.C., D.K. and G.R.; supervision, R.S., G.R. and P.R.; project administration, A.K.; funding acquisition, A.K., T.C.-K.Y. and P.R. All authors have read and agreed to the published version of the manuscript.

Funding

This project has received funding from the European Union’s Horizon 2020 research and innovation program under the Marie Skłodowska-Curie grant agreement No 778070—TransFerr—H2020-MSCA-RISE-2017.

Institutional Review Board Statement

Not applicable.

Data Availability Statement

Data Availability Statements are available in section.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Fiebig, M.; Lottermoser, T.; Meier, D.; Trassin, M. The evolution of multiferroics. Nat. Rev. Mater. 2016, 1, 16046. [Google Scholar] [CrossRef]
  2. Wang, W.; Zhao, J.; Wang, W.; Gai, Z.; Balke, N.; Chi, M.; Lee, H.N.; Tian, W.; Zhu, L.; Cheng, X.; et al. Room-temperature multiferroic hexagonal LuFeO3 films. Phys. Rev. Lett. 2013, 110, 237601. [Google Scholar] [CrossRef] [PubMed]
  3. Cao, S.; Zhang, X.; Paudel, T.R.; Sinha, K.; Wang, X.; Jiang, X.; Wang, W.; Brutsche, S.; Wang, J.; Ryan, P.J.; et al. On the structural origin of the single-ion magnetic anisotropy in LuFeO3. J. Phys. Condens. Matter 2016, 28, 156001. [Google Scholar] [CrossRef] [PubMed]
  4. Pakalniškis, A.; Alikin, D.O.; Turygin, A.P.; Zhaludkevich, A.L.; Silibin, M.V.; Zhaludkevich, D.V.; Niaura, G.; Zarkov, A.; Skaudžius, R.; Karpinsky, D.V.; et al. Crystal Structure and Concentration-Driven Phase Transitions in Lu(1−x)ScxFeO3 (0 ≤ x ≤ 1) Prepared by the Sol–Gel Method. Materials 2022, 15, 1048. [Google Scholar] [CrossRef] [PubMed]
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Article Metrics

Citations

Article Access Statistics

Multiple requests from the same IP address are counted as one view.