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dc.contributor.authorChoi, Y. J.en_US
dc.contributor.authorOkamoto, J.en_US
dc.contributor.authorHuang, D. J.en_US
dc.contributor.authorChao, K. S.en_US
dc.contributor.authorLin, H. J.en_US
dc.contributor.authorChen, C. T.en_US
dc.contributor.authorvan Veenendaal, M.en_US
dc.contributor.authorKaplan, T. A.en_US
dc.contributor.authorCheong, S-W.en_US
dc.date.accessioned2014-12-08T15:10:00Z-
dc.date.available2014-12-08T15:10:00Z-
dc.date.issued2009-02-13en_US
dc.identifier.issn0031-9007en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevLett.102.067601en_US
dc.identifier.urihttp://hdl.handle.net/11536/7632-
dc.description.abstractWe report the unexpected evolution, with thermal and magnetic-field (H) variations, of the interrelation between the polarization P, magnetization M, and spiral wave vector Q in CoCr(2)O(4), which has a ferrimagnetic conical-spiral magnetic order. For example, P suddenly jumps and changes its sign at the magnetic lock-in transition (T(L)) with thermal variation, or with isothermal variation of H (without changing its direction) at T(L), which surprisingly occurs without change in spiral handedness (i.e., the sign of Q). The presence of multiple spiral sublattices may be behind this unusual behavior.en_US
dc.language.isoen_USen_US
dc.titleThermally or Magnetically Induced Polarization Reversal in the Multiferroic CoCr(2)O(4)en_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevLett.102.067601en_US
dc.identifier.journalPHYSICAL REVIEW LETTERSen_US
dc.citation.volume102en_US
dc.citation.issue6en_US
dc.citation.spageen_US
dc.citation.epageen_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
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