2018
DOI: 10.1103/physrevb.98.035149
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Excitonic dispersion of the intermediate spin state in LaCoO3 revealed by resonant inelastic x-ray scattering

Abstract: We report Co L3-edge resonant inelastic X-ray scattering on LaCoO3 at 20 K. We observe excitations with sizable dispersion that we identify as intermediate-spin (IS) states. Theoretical calculations that treat the IS states as mobile excitons propagating on the low-spin (LS) background support the interpretation. The present result shows that mobility substantially reduces the energy of IS excitations in part of the Brillouin zone, which makes them important players in the low-energy physics of LaCoO3 together… Show more

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Cited by 20 publications
(28 citation statements)
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“…The comparison of L 2,3 -edge spectra in this study to references confirms the presence of Co 2+ in stable high-spin (HS) state 14 , Ni 3+ in the low-spin (LS) configuration 17 and different spin states of Co 3+ . Spin states of Co 3+ in LaCoO 3 have been subject to extensive debate in literature 13,18 , as Co 3+ may occur in the LS ground state, the first excited HS state, or excited states with intermediate spin 19 . Obtained spectra are equivalent to previous results related to a mixture of LS and HS states and spin state abundance was thus determined by a least squares fit of a linear combination of two reference spectra 13 representing a pure LS configuration and a mixed LS-HS state.…”
Section: Resultsmentioning
confidence: 99%
“…The comparison of L 2,3 -edge spectra in this study to references confirms the presence of Co 2+ in stable high-spin (HS) state 14 , Ni 3+ in the low-spin (LS) configuration 17 and different spin states of Co 3+ . Spin states of Co 3+ in LaCoO 3 have been subject to extensive debate in literature 13,18 , as Co 3+ may occur in the LS ground state, the first excited HS state, or excited states with intermediate spin 19 . Obtained spectra are equivalent to previous results related to a mixture of LS and HS states and spin state abundance was thus determined by a least squares fit of a linear combination of two reference spectra 13 representing a pure LS configuration and a mixed LS-HS state.…”
Section: Resultsmentioning
confidence: 99%
“…Further details of the experiments can be found in the Supplemental Material of Ref. [42]. Figure 3(a) compares the fluorescence yield XAS spectra acquired from two orthogonal linear polarized incident beams.…”
Section: The 2p3d Rixs Experimentsmentioning
confidence: 99%
“…In an effort to contribute to the debate about the origin of magnetism in LaCoO 3 , we employ 2p3d resonant inelastic x-ray scattering (2p3d RIXS) to study the complex electronic configuration of the Co ions in a LaCoO 3 single crystal and strained thin films. 2p3d RIXS probes both the local [26][27][28][29][30][31][32][33][34] and collective excitations [35][36][37][38][39][40][41][42], including small lattice distortions [43][44][45]. In the case of LaCoO 3 , the 2p3d RIXS process in the ionic limit can be described as 3d 6 > 2p 5 3d 7 > 3d 6 transitions of Co 3+ ions, which allows us to distinguish the spin-state manifolds.…”
Section: Introductionmentioning
confidence: 99%
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“…In the EI theories, the intermediate‐spin (IS) state generates the spatially mobile exciton as the source of dispersive spin‐state excitations . By contrast, the HS state is described as an immobile bi‐exciton consisting of two types of IS excitons with different site‐hopping directionality and results in the nondispersive excitations 6c,28. In this scheme, the HS condensation ranging multiple sites would lead to a novel bi‐excitonic insulating (bi‐EI) state with dual nature of immobility (localization) and site coherence (itinerancy).…”
mentioning
confidence: 99%