Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/10191
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dc.contributor.authorSahoo, S.en_US
dc.contributor.authorBabu, S.en_US
dc.contributor.authorHissariya, R.en_US
dc.contributor.authorROUT, D.en_US
dc.contributor.authorSINGH, S.en_US
dc.contributor.authorAbrudan, R.en_US
dc.contributor.authorRadu, F.en_US
dc.contributor.authorSaini, D.en_US
dc.contributor.authorMandal, D.en_US
dc.contributor.authorMishra, S. K.en_US
dc.date.accessioned2025-06-23T05:14:27Z
dc.date.available2025-06-23T05:14:27Z
dc.date.issued2025-12en_US
dc.identifier.citationJournal of Physics and Chemistry of Solids, 207, 112891.en_US
dc.identifier.issn0022-3697en_US
dc.identifier.issn1879-2553en_US
dc.identifier.urihttps://doi.org/10.1016/j.jpcs.2025.112891en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/10191
dc.description.abstractFuturistic multi-state storage devices and energy-efficient data storage sensors depend on advanced functional materials that manifest both spin and charge ordering. Here, we report the growth of SmMn0.25Fe0.75O3 (SMFO) single crystals, which crystallize in an orthorhombic structure (space group: Pbnm), as determined through measurements of temperature-dependent X-ray diffraction (XRD). The SMFO crystals display varying physical properties due to modulation of the spin reorientation transition (SRT) Γ4 → Γ2 at 382 K, which is relatively lower than the 450 K transition reported in pristine SmFeO3. Moreover, the addition of Mn (25 %) induces a new spin reorientation (TSR1: Γ2 → Γ1) occurring at 175 K. The observed exchange-bias effect in the SMFO crystal shows a divergence at the onset of spin reorientation temperature. The spin canting angle in SMFO is characterized within the context of mixed ferromagnetic and antiferromagnetic domains. We further elaborate direct correlation between anisotropic lattice compression and the spin canting angles. The mutual competing 3d-3d and 3d-4f spin exchange interactions between the magnetic moments of Sm3+ ions and Fe3+ (Mn3+) ions, which results in minimal lattice distortions that break inversion symmetry. This leads to the Dzyaloshinskii-Moriya (D-M) interaction that further induces a net electric dipole moment. These experimental findings indicate that competing exchange interactions are crucial in controlling the exchange bias, spin-anisotropy, lattice distortion, and ferroelectricity, which are beneficial for the development of functional devices and their applications.en_US
dc.language.isoenen_US
dc.publisherElsevier B.V.en_US
dc.subjectExchange biasen_US
dc.subjectExchange interactionsen_US
dc.subjectSpin-reorientationen_US
dc.subjectPhase transitionsen_US
dc.subjectOrthoferritesen_US
dc.subjectMultistate Memory Devicesen_US
dc.subject2025-JUN-WEEK3en_US
dc.subjectTOC-JUN-2025en_US
dc.subject2025en_US
dc.titleModulation of spin reorientation and exchange bias in SmMn0.25Fe0.75O3 orthoferrite single crystalen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleJournal of Physics and Chemistry of Solidsen_US
dc.publication.originofpublisherForeignen_US
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