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Thermally or Magnetically Induced Polarization Reversal in the Multiferroic CoCr2O4

dc.citation.epage0en_US
dc.citation.issue6en_US
dc.citation.spage0en_US
dc.citation.volume102en_US
dc.citation.woscount127en_US
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.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.date.accessioned2019-04-03T06:42:36Z
dc.date.available2019-04-03T06:42:36Z
dc.date.issued2009-02-13en_US
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 CoCr2O4, 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.identifier.doi10.1103/PhysRevLett.102.067601en_US
dc.identifier.issn0031-9007en_US
dc.identifier.journalPHYSICAL REVIEW LETTERSen_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevLett.102.067601en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/149745
dc.identifier.wosnumberWOS:000263389500066en_US
dc.language.isoen_USen_US
dc.titleThermally or Magnetically Induced Polarization Reversal in the Multiferroic CoCr2O4en_US
dc.typeArticleen_US

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