Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/2798
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dc.contributor.authorKumar, Sanjeev-
dc.date.accessioned2020-12-08T05:58:49Z-
dc.date.available2020-12-08T05:58:49Z-
dc.date.issued2013-
dc.identifier.citationNature Communications,4.en_US
dc.identifier.other10.1038/ncomms3511-
dc.identifier.urihttps://www.nature.com/articles/ncomms3511-
dc.identifier.urihttp://hdl.handle.net/123456789/2798-
dc.descriptionOnly IISERM authors are available in the record.-
dc.description.abstractMultiferroic materials, in which ferroelectric and magnetic ordering coexist, are of fundamental interest for the development of multi-state memory devices that allow for electrical writing and non-destructive magnetic readout operation. The great challenge is to create multiferroic materials that operate at room temperature and have a large ferroelectric polarization P. Cupric oxide, CuO, is promising because it exhibits a significant polarization, that is, P~0.1 μC cm−2, for a spin-spiral multiferroic. Unfortunately, CuO is only ferroelectric in a temperature range of 20 K, from 210 to 230 K. Here, by using a combination of density functional theory and Monte Carlo calculations, we establish that pressure-driven phase competition induces a giant stabilization of the multiferroic phase of CuO, which at 20–40 GPa becomes stable in a domain larger than 300 K, from 0 to T>300 K. Thus, under high pressure, CuO is predicted to be a room-temperature multiferroic with large polarization.en_US
dc.language.isoenen_US
dc.publisherNatureen_US
dc.subjectMaterialsen_US
dc.subjectMagneticen_US
dc.subjectMultiferroicen_US
dc.subjectFerroelectricen_US
dc.titleRoom-temperature spin-spiral multiferroicity in high-pressure cupric oxideen_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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