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dc.contributor.authorChen, J. M.en_US
dc.contributor.authorLee, J. M.en_US
dc.contributor.authorHuang, S. W.en_US
dc.contributor.authorLu, K. T.en_US
dc.contributor.authorJeng, H. T.en_US
dc.contributor.authorChen, C. K.en_US
dc.contributor.authorHaw, S. C.en_US
dc.contributor.authorChou, T. L.en_US
dc.contributor.authorChen, S. A.en_US
dc.contributor.authorHiraoka, N.en_US
dc.contributor.authorIshii, H.en_US
dc.contributor.authorTsuei, K. D.en_US
dc.contributor.authorYang, T. J.en_US
dc.date.accessioned2019-04-03T06:38:37Z-
dc.date.available2019-04-03T06:38:37Z-
dc.date.issued2010-09-27en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.82.094442en_US
dc.identifier.urihttp://hdl.handle.net/11536/150045-
dc.description.abstractMn 3d valence states and elementary electronic excitations in single-crystalline TbMnO3 were probed with resonant inelastic x-ray scattering (RIXS) (or resonant x-ray emission spectroscopy, RXES), polarized x-ray absorption spectra and ab initio electron-structure calculations. Polarized Mn K-edge x-ray absorption spectra of TbMnO3 crystals exhibit a significant anisotropy along three crystallographic directions, particularly for the white-line region. The 1s3p-RXES spectra obtained at the Mn K edge reveal that the quadrupolar Raman regime is restricted predominantly to below the pre-edge peak whereas the fluorescence regime starts from the first pre-edge peak of 1s -> 3d transitions, indicating a relatively delocalized character of unoccupied Mn 3d states. The additional K beta emission profile at energy loss similar to 62 eV is attributed to the off-site dipole Mn 1s-Mn' 3d and/or Mn 1s-Tb 5d transitions, originating from hybridization between Mn 4p states and neighboring Mn' 3d/Tb 5d states. The off-site dipole transition makes a considerable contribution to the pre-edge region of Mn K-edge spectrum. Three prominent RIXS features at similar to 2.9, 7, and 11 eV were observed. Based on GGA+U calculations, the 7 eV region corresponds to transitions from O 2p states to unoccupied minority Mn 3d states, whereas the 11 eV band is ascribed to transitions from the O 2p band to the empty Tb 5d band. The broad 2.9 eV band is attributed to the coexistence of on-site Mn 3d-Mn 3d and off-site Mn 3d-Mn' 3d transitions.en_US
dc.language.isoen_USen_US
dc.titleIntra- and intersite electronic excitations in multiferroic TbMnO3 probed by resonant inelastic x-ray scatteringen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.82.094442en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume82en_US
dc.citation.issue9en_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:000282167600001en_US
dc.citation.woscount12en_US
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