Please use this identifier to cite or link to this item: https://libjncir.jncasr.ac.in/xmlui/handle/10572/74
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dc.contributor.authorSerrao, Claudy Rayan-
dc.contributor.authorKrupanidhi, S B-
dc.contributor.authorBhattacharjee, Joydeep-
dc.contributor.authorWaghmare, Umesh V-
dc.contributor.authorKundu, Asish K-
dc.contributor.authorRao, C N R-
dc.date.accessioned2011-03-22T08:38:49Z-
dc.date.available2011-03-22T08:38:49Z-
dc.date.issued2006-10-01-
dc.identifier0021-8979en_US
dc.identifier.citationJournal of Applied Physics 100(7) , 076104-1-2 (2006)en_US
dc.identifier.urihttps://libjncir.jncasr.ac.in/xmlui/10572/74-
dc.description.abstractInMnO3 which has a hexagonal structure similar to that of YMnO3 is found to show a canted antiferromagnetic behavior below 50 K (T-N) and a ferroelectric (FE) transition at 500 K accompanied by hystersis. We have determined the structure, polarization, and energetics of the FE and paraelectric (PE) phases of InMnO3 using first-principles density functional theory calculations based on pseudopotentials and a plane-wave basis, and find the polarization of the PE phase to be a half-integer quantum. The difference in polarization of the FE and PE phases calculated along a simple path is different from the absolute value of polarization of the FE phase. A weak piezoelectric response is exhibited by InMnO3 to uniaxial strain. (c) 2006 American Institute of Physics.en_US
dc.description.urihttp://dx.doi.org/10.1063/1.2356093en_US
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2006 American Institute of Physicsen_US
dc.subjectMagnetic Ferroelectricsen_US
dc.subjectYmno3en_US
dc.subjectPolarizationen_US
dc.subjectTransitionen_US
dc.titleInMnO3: A biferroicen_US
dc.typeArticleen_US
Appears in Collections:Research Papers (Prof. C.N.R. Rao)

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