Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/9581
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dc.contributor.authorCHATURVEDI, SMITAen_US
dc.contributor.authorShyam, Priyanken_US
dc.contributor.authorLiu, Yingen_US
dc.contributor.authorSrinivasan, Gopalanen_US
dc.date.accessioned2025-04-15T06:54:17Z-
dc.date.available2025-04-15T06:54:17Z-
dc.date.issued2024-05en_US
dc.identifier.citationJounral of the American Ceramic Society, 107(05), 3368-3379.en_US
dc.identifier.issn1551-2916en_US
dc.identifier.issn0002-7820en_US
dc.identifier.urihttps://doi.org/10.1111/jace.19663en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/9581-
dc.description.abstractThe effect of ionic radii sizes on magnetostriction is studied in relation to structural and magnetic properties. To explore the effect of the chemical pressure, nanoparticles of rare-earth (RE) orthoferrites, SmFeO3, DyFeO3, HoFeO3, and LuFeO3 are studied using X-ray diffraction, field emission scanning electron microscopy, and Raman spectroscopy. Magnetic and magnetostriction measurements are also performed. In these orthoferrites, the coordination of the RE ion is eightfold, whereas the RE ionic radii are significantly different, which directly influences the structural parameters. The distortion of FeO6 octahedra is observed as a result of changing chemical pressure within the lattice. The different magnitudes of magnetostriction in RE orthoferrites can be attributed to the different degrees of distortion of FeO6 octahedra, R–O dynamics, and spin–orbit interactions in the system. The maximum value of magnetostriction (∼ 19 ppm) and magnetization at 2 K (30.64 emu/g) is demonstrated by HoFeO3. Comparison of structural parameters of the samples to their respective bulk counterparts indicated relative structural distortion in nanoparticles.en_US
dc.language.isoenen_US
dc.publisherAmerican Ceramic Societyen_US
dc.subjectPhysicsen_US
dc.subject2024en_US
dc.titleManifestation of chemical pressure: Magnetism and magnetostriction in nanoscale RFeO3 (R = Sm, Dy, Ho, and Lu)en_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleJounral of the American Ceramic Societyen_US
dc.publication.originofpublisherForeignen_US
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