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dc.contributor.authorOkamoto, J.en_US
dc.contributor.authorHuang, D. J.en_US
dc.contributor.authorMou, C. -Y.en_US
dc.contributor.authorChao, K. S.en_US
dc.contributor.authorLin, H. -J.en_US
dc.contributor.authorPark, S.en_US
dc.contributor.authorCheong, S-W.en_US
dc.contributor.authorChen, C. T.en_US
dc.date.accessioned2019-04-03T06:44:38Z-
dc.date.available2019-04-03T06:44:38Z-
dc.date.issued2007-04-13en_US
dc.identifier.issn0031-9007en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevLett.98.157202en_US
dc.identifier.urihttp://hdl.handle.net/11536/10917-
dc.description.abstractBased on measurements of soft-x-ray magnetic scattering and symmetry considerations, we demonstrate that the magnetoelectric effect in TbMn2O5 arises from an internal field determined by (S) over right arrow ((q) over right arrow) x (s) over right arrow (-(q) over right arrow) with (S) over right arrow ((q) over right arrow) being the magnetization at modulation vector (q) over right arrow, whereas the magnetoelastic effect in the exchange energy governs the response to external electric fields. Our results set fundamental symmetry constraints on the microscopic mechanism of multiferroicity in frustrated magnets.en_US
dc.language.isoen_USen_US
dc.titleSymmetry of multiferroicity in a frustrated magnet TbMn2O5en_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevLett.98.157202en_US
dc.identifier.journalPHYSICAL REVIEW LETTERSen_US
dc.citation.volume98en_US
dc.citation.issue15en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000245691400055en_US
dc.citation.woscount32en_US
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