2009
DOI: 10.1103/physrevb.79.035110
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Resonant soft x-ray inelastic scattering and soft x-ray emission study of the electronic structure ofα-MoO3

Abstract: The electronic structure of quasi-low-dimensional solids is a topic of enduring interest due to the complex many-body interactions that exist in such materials and their resulting exotic physical properties. A well studied class of such materials is the quasi-low-dimensional metals known collectively as molybdenum oxide bronzes. These materials are all derived from the band insulator ␣-MoO 3 . We report here a study of the electronic structure of ␣-MoO 3 using resonant inelastic x-ray scattering and soft x-ray… Show more

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Cited by 11 publications
(11 citation statements)
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“…As the oxygen ratio increased, the O 2p peak at ca 5 eV evolved by hybridization with Cu 3d. These values are 4.5, and ~6 eV below the Fermi level [23]. The increase of the partial density of state at 5 eV indicates Cu was oxidized.…”
Section: Resultsmentioning
confidence: 96%
“…As the oxygen ratio increased, the O 2p peak at ca 5 eV evolved by hybridization with Cu 3d. These values are 4.5, and ~6 eV below the Fermi level [23]. The increase of the partial density of state at 5 eV indicates Cu was oxidized.…”
Section: Resultsmentioning
confidence: 96%
“…21,27,28,47,65 In order for the incident-beam polarization to have a large c-axis component ͑as in Ref. 35͒ while maintaining a ϳ90°scatter-ing angle, the measurements were carried out at the Q positions of ͑3.5 0 6͒, ͑3.5 0.25 6͒, ͑3.5,0.5,6͒, and ͑3 0 8.5͒ for reduced momentum q of ͑ 0͒, ͑ / 2͒, ͑ ͒, and ͑0 0͒, respectively.…”
Section: Methodsmentioning
confidence: 99%
“…The scattering plane was horizontal, with the incident polarization parallel to the scattering plane (π-polarization) and the scattering angle was set to nearly 90 degrees, thereby suppressing the background from the elastic peak. 21,27,28,47,65 In order for the incident beam polarization to have a large c-axis component (as in Ref. 35) while maintaining a ∼90 degree scattering angle, the measurements were carried out at the Q-positions of (3.5 0 6), (3.5 0.25 6), (3.5,0.5,6) and (3 0 8.5) for reduced momentum q of (π 0), (π π/2), (π π) and (0 0), respectively.…”
Section: Methodsmentioning
confidence: 99%
“…The possibility of measuring momentum dependence at the Oxygen K edge has also been suggested (Okada and Kotani, 2007). Learmonth et al (2009) used oxygen K-edge RIXS to probe the electronic structure of the band insulator α-MoO 3 and observe that when the incident energy is resonantly tuned to the π states at the Fermi level, momentum selectivity allows the observation of states only near certain symmetry points reflecting the highly anisotropic electronic structure of α-MoO 3 .…”
Section: Early Workmentioning
confidence: 99%