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Article: Phonon softening and forbidden mode in Na0.5 Co O2 observed by Raman scattering

TitlePhonon softening and forbidden mode in Na0.5 Co O2 observed by Raman scattering
Authors
Issue Date2008
Citation
Physical Review B - Condensed Matter and Materials Physics, 2008, v. 77, n. 4 How to Cite?
AbstractPolarized Raman scattering measurements have been performed on Na0.5 Co O2 single crystal from 8 to 305 K. Both the A1g and E1g phonon modes show a softening below Tc1 ≈ 83 K. Additionally, the A1g phonon mode, which is forbidden in the scattering geometry of cross polarization for the triangular Co O2 layers, appears below Tc1. In contrast, the metal-insulator transition at Tc2 ≈ 46 K has only secondary effect on the Raman spectra. The phonon softening and the "forbidden" Raman intensity follow closely magnetic order parameter and the gap function at the Fermi surface, indicating that the distortion of Co O6 octahedra at Tc1, instead of the Na ordering at ∼350 K, is the relevant structural component of the 83 K phase transition. © 2008 The American Physical Society.
Persistent Identifierhttp://hdl.handle.net/10722/254510
ISSN
2014 Impact Factor: 3.736
2015 SCImago Journal Rankings: 1.933

 

DC FieldValueLanguage
dc.contributor.authorZhang, Qingming-
dc.contributor.authorAn, Ming-
dc.contributor.authorYuan, Shikui-
dc.contributor.authorWu, Yong-
dc.contributor.authorWu, Dong-
dc.contributor.authorLuo, Jianlin-
dc.contributor.authorWang, Nanlin-
dc.contributor.authorBao, Wei-
dc.contributor.authorWang, Yening-
dc.date.accessioned2018-06-19T15:40:45Z-
dc.date.available2018-06-19T15:40:45Z-
dc.date.issued2008-
dc.identifier.citationPhysical Review B - Condensed Matter and Materials Physics, 2008, v. 77, n. 4-
dc.identifier.issn1098-0121-
dc.identifier.urihttp://hdl.handle.net/10722/254510-
dc.description.abstractPolarized Raman scattering measurements have been performed on Na0.5 Co O2 single crystal from 8 to 305 K. Both the A1g and E1g phonon modes show a softening below Tc1 ≈ 83 K. Additionally, the A1g phonon mode, which is forbidden in the scattering geometry of cross polarization for the triangular Co O2 layers, appears below Tc1. In contrast, the metal-insulator transition at Tc2 ≈ 46 K has only secondary effect on the Raman spectra. The phonon softening and the "forbidden" Raman intensity follow closely magnetic order parameter and the gap function at the Fermi surface, indicating that the distortion of Co O6 octahedra at Tc1, instead of the Na ordering at ∼350 K, is the relevant structural component of the 83 K phase transition. © 2008 The American Physical Society.-
dc.languageeng-
dc.relation.ispartofPhysical Review B - Condensed Matter and Materials Physics-
dc.titlePhonon softening and forbidden mode in Na0.5 Co O2 observed by Raman scattering-
dc.typeArticle-
dc.description.natureLink_to_subscribed_fulltext-
dc.identifier.doi10.1103/PhysRevB.77.045110-
dc.identifier.scopuseid_2-s2.0-38049107397-
dc.identifier.volume77-
dc.identifier.issue4-
dc.identifier.spagenull-
dc.identifier.epagenull-
dc.identifier.eissn1550-235X-

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