Variation in the dielectric and magnetic characteristics of multiferroic LuFeO3 as a result of cobalt substitution at Fe sites

dc.authorid0000-0002-0463-4292
dc.authorid0000-0001-6193-0373
dc.authorid0000-0001-9724-7664
dc.contributor.authorPolat, O.
dc.contributor.authorCoşkun, M.
dc.contributor.authorYildirim, Y.
dc.contributor.authorRoupcova, P.
dc.contributor.authorSobola, D.
dc.contributor.authorSen, C.
dc.contributor.authorDurmuş, Zehra
dc.date.accessioned2025-05-10T19:50:03Z
dc.date.issued2023
dc.departmentİstanbul Medeniyet Üniversitesi
dc.description.abstractDue to its electrical, magnetic, and optical characteristics, LuFeO3 (LFO) has caught the scientific community's interest. In this study, the powders of LFO, LuFe0.95Co0.05O3, and LuFe0.90Co0.10O3 samples were prepared by using the well-known solid-state approach. The crystalline structure of the fabricated samples was examined by an X-ray diffractometer (XRD). It was found that the samples display secondary phases such as Lu2O3, Lutetium Tetraoxodiferrate, and Wustite. It was shown by scanning electron microscope (SEM) that particle size decreases with Co doping. X-ray photoelectron spectroscopy (XPS) determined oxidation states for Fe and Co. It was presented that Fe has a mixture of 2 + and + 3 valance states in the LFO sample. Although LuFe0.95Co0.05O3 has only the 3 + state, LuFe0.90Co0.10O3 sample has coexisting metallic and 3 + states. The conductivity and dielectric constant of the undoped LFO sample were higher than those of Co doped LFO samples. A decrease in both the dielectric constant and conductivity was associated with a lack of Fe2+ ions and lattice distortions. Furthermore, it was argued that several conduction models must be developed to explain the conduction process in the analyzed samples. Magnetic experiments using a vibrating sample magnetometer (VSM) revealed that Co doping raises Mr values. We discuss that this increase in Mr values could be related to i) variations in the inclined angles of Fe3+ moments and ii) the growth of magnetocrystalline anisotropy's energy.
dc.description.sponsorshipScientific and Technological Research Council of Turkey (TUBITAK) [116F025]; MEYS CR [LM 2018110]; Istanbul Medeniyet University Science and Advanced Technology Research Center (IMU-BILTAM)
dc.description.sponsorshipThis work was supported by The Scientific and Technological Research Council of Turkey (TUBITAK) through Grant No: 116F025. We acknowledge CEITEC Nano Research Infrastructure supported by MEYS CR (LM 2018110) and Istanbul Medeniyet University Science and Advanced Technology Research Center (IMU-BILTAM) .
dc.identifier.doi10.1016/j.jallcom.2023.170939
dc.identifier.issn0925-8388
dc.identifier.issn1873-4669
dc.identifier.scopus2-s2.0-85164365333
dc.identifier.scopusqualityQ1
dc.identifier.urihttps://doi.org/10.1016/j.jallcom.2023.170939
dc.identifier.urihttps://hdl.handle.net/20.500.14730/12234
dc.identifier.volume963
dc.identifier.wosWOS:001037809400001
dc.identifier.wosqualityQ1
dc.indekslendigikaynakWeb of Science
dc.indekslendigikaynakScopus
dc.language.isoen
dc.publisherElsevier Science Sa
dc.relation.ispartofJournal of Alloys and Compounds
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.snmzKA_WOS_20250302
dc.subjectSolid-state reaction
dc.subjectLuFeO3
dc.subjectCo doping
dc.subjectDielectric properties
dc.subjectConductivity
dc.subjectMagnetic properties
dc.titleVariation in the dielectric and magnetic characteristics of multiferroic LuFeO3 as a result of cobalt substitution at Fe sites
dc.typeArticle

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