Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1107
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dc.contributor.authorPANJA, SOUMENDRA NATHen_US
dc.contributor.authorHARNAGEA, LUMINITAen_US
dc.contributor.authorKUMAR, JITENDERen_US
dc.contributor.authorMukharjee, I. P. K.en_US
dc.contributor.authorNath, R.en_US
dc.contributor.authorNigam, A. K.en_US
dc.contributor.authorNAIR, SUNILen_US
dc.date.accessioned2018-07-26T12:00:03Z
dc.date.available2018-07-26T12:00:03Z
dc.date.issued2018-07en_US
dc.identifier.citationPhysical Review B., 98(2).en_US
dc.identifier.issn2469-9969en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1107
dc.identifier.urihttps://doi.org/10.1103/PhysRevB.98.024410en_US
dc.description.abstractWe report on the magnetic, thermodynamic, dielectric, and pyroelectric measurements on the hitherto unreported Fe4Ta2O9 . This system is seen to exhibit a series of magnetic transitions, many of which are coupled to the emergence of ferroelectric order, making Fe4Ta2O9 the only genuine multiferroic in its material class. We suggest that the observed properties arise as a consequence of an effective reduction in the dimensionality of the magnetic lattice, with the magnetically active Fe2+ ions preferentially occupying a quasi-two-dimensional buckled honeycomb structure. The low-temperature H-T phase diagram of Fe4Ta2O9 reveals a rich variety of coupled magnetic and ferroelectric phases similar to that observed in the distorted kagome systems.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectTransitionen_US
dc.subjectTOC-JULY-2018en_US
dc.subject2018en_US
dc.titleCoupled magnetic and ferroelectric states in the distorted honeycomb system Fe4Ta2O9en_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Ben_US
dc.publication.originofpublisherForeignen_US
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