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Presence of Induced Weak Ferromagnetism in Fe-Substituted YFe(x)Cr(1−x)O(3) Crystalline Compounds

Fe-substituted YFe(x)Cr(1−x)O(3) crystalline compounds show promising magnetic and multiferroic properties. Here we report the synthesis and characterization of several compositions from this series. Using the autocombustion route, various compositions (x = 0.25, 0.50, 0.6, 0.75, 0.9, and 1) were sy...

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Detalles Bibliográficos
Autores principales: Salazar-Rodriguez, Roberto, Aliaga Guerra, Domingo, Greneche, Jean-Marc, Taddei, Keith M., Checca-Huaman, Noemi-Raquel, Passamani, Edson C., Ramos-Guivar, Juan A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9565242/
https://www.ncbi.nlm.nih.gov/pubmed/36234644
http://dx.doi.org/10.3390/nano12193516
Descripción
Sumario:Fe-substituted YFe(x)Cr(1−x)O(3) crystalline compounds show promising magnetic and multiferroic properties. Here we report the synthesis and characterization of several compositions from this series. Using the autocombustion route, various compositions (x = 0.25, 0.50, 0.6, 0.75, 0.9, and 1) were synthesized as high-quality crystalline powders. In order to obtain microscopic and atomic information about their structure and magnetism, characterization was performed using room temperature X-ray diffraction and energy dispersion analysis as well as temperature-dependent neutron diffraction, magnetometry, and (57)Fe Mössbauer spectrometry. Rietveld analysis of the diffraction data revealed a crystallite size of 84 (8) nm for YFeO(3), while energy dispersion analysis indicated compositions close to the nominal compositions. The magnetic results suggested an enhancement of the weak ferromagnetism for the YFeO(3) phase due to two contributions. First, a high magnetocrystalline anisotropy was associated with the crystalline character that favored a unique high canting angle of the antiferromagnetic phase (13°), as indicated by the neutron diffraction analysis. This was also evidenced by the high magnetic hysteresis curves up to 90 kOe by a remarkable high critical coercivity value of 46.7 kOe at room temperature. Second, the Dzyaloshinskii–Moriya interactions between homogenous and heterogeneous magnetic pairs resulted from the inhomogeneous distribution of Fe(3+) and Cr(3+) ions, as indicated by (57)Fe Mössbauer studies. Together, these results point to new methods of controlling the magnetic properties of these materials.