2001
DOI: 10.1103/physrevb.64.075112
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Electronic structure ofCuGeO3:Charge excitations between zero and one dimension

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Cited by 16 publications
(19 citation statements)
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“…A similar structure, followed at high photon energies by a region of strong absorption ascribed to transitions to the empty states above the charge transfer gap, is also present in transmission EELS spectra, 10 in the optical spectra, 11 and in x-ray Raman scattering spectra. 12 The energy position and the strong dependence of this peak on light polarization suggest that this structure can be related to the Zhang-Rice-like exciton.…”
mentioning
confidence: 56%
See 1 more Smart Citation
“…A similar structure, followed at high photon energies by a region of strong absorption ascribed to transitions to the empty states above the charge transfer gap, is also present in transmission EELS spectra, 10 in the optical spectra, 11 and in x-ray Raman scattering spectra. 12 The energy position and the strong dependence of this peak on light polarization suggest that this structure can be related to the Zhang-Rice-like exciton.…”
mentioning
confidence: 56%
“…Due to the hybridization between Cu 3d and O 2p orbitals and to the strong dependence of the charge transfer excitation on the geometry of the Cu-O plaquettes, the picture of charge transfer excitation alone can not fully account for the fine structure details of the observed spectrum. Indeed, as pointed out by Zhang and Ng 15 and, successively, by Atzkern et al, 10 depending on Cu-O hybridization and bond geometry, the CT excitation picture should be completed by an analysis of the hole delocalization. Zhang and Ng 15 describe the CT-exciton in the insulating CuO2 plane and conclude that a very complex exciton is formed, consisting of a 3d electron on copper and a nearby Cu-O singlet.…”
mentioning
confidence: 96%
“…In particular, we obtain n ph /n Cu ≈Φ pump α/n Cu ≃0.1-0.2%, being α=500 cm −1 . Considering the rapid delocalization of each hole within about 5 neighboring plaquettes, 13 it is possible to conclude that, during the pulse duration, ∼0.5-1% of the Cu−O 6 units are driven to the excited state where the correlated 3d bands are locally filled by an electron and a hole is shared among the O-2p orbitals and the Cu-3d levels of the neighboring plaquettes (see Fig. 1d), possibly altering both the interaction U and the transfer integral T pd , and leaving the system in a metastable non-thermal phase.…”
Section: Resultsmentioning
confidence: 99%
“…The shoulder in the absorption coefficient at 3.1-3-2 eV (see Fig. 1c) is attributed to a superposition of plasmons related to transitions from the ground state, being 72% of the hole density localized on Cu atoms, into a delocalized final state with a high occupation probability of the neighbor plaquettes, 13,15 as shown in Fig. 1d.…”
Section: 18mentioning
confidence: 99%
“…For quasi-one dimensional compounds a large values of ε ∞ ∼ 8 was taken in Refs. 19,20. This means that the rest of the solid strongly screens the long-range part of the Coulomb interaction between electrons that enter the Hubbard model.…”
Section: Resultsmentioning
confidence: 99%