2009
DOI: 10.1103/physrevb.79.205211
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Band gap, electronic structure, and surface electron accumulation of cubic and rhombohedralIn2O3

Abstract: The bulk and surface electronic structure of In 2 O 3 has proved controversial, prompting the current combined experimental and theoretical investigation. The band gap of single-crystalline In 2 O 3 is determined as 2.93Ϯ 0.15 and 3.02Ϯ 0.15 eV for the cubic bixbyite and rhombohedral polymorphs, respectively. The valence-band density of states is investigated from x-ray photoemission spectroscopy measurements and density-functional theory calculations. These show excellent agreement, supporting the absence of … Show more

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Cited by 383 publications
(233 citation statements)
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“…Zhang et al [136] employed energy-dependent photoemission, utilizing the inherent variation in surface specificity with photon energy to support this conclusion, providing spectroscopic confirmation of the increased electron density at In 2 O 3 surfaces. Via extrinsic Sn-doping to increase the bulk carrier concentration, it is possible to quench the electron accumulation [134,135]. This provides a mechanism to reconcile these recent results with earlier studies which suggested a depletion of electrons at the surface [131][132][133].…”
Section: Surface Conductivitysupporting
confidence: 63%
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“…Zhang et al [136] employed energy-dependent photoemission, utilizing the inherent variation in surface specificity with photon energy to support this conclusion, providing spectroscopic confirmation of the increased electron density at In 2 O 3 surfaces. Via extrinsic Sn-doping to increase the bulk carrier concentration, it is possible to quench the electron accumulation [134,135]. This provides a mechanism to reconcile these recent results with earlier studies which suggested a depletion of electrons at the surface [131][132][133].…”
Section: Surface Conductivitysupporting
confidence: 63%
“…8(d)). Such a surface electron accumulation was found to be remarkably independent of surface orientation or even bulk polymorph, with a very similar pinning level of the surface Fermi level, and resulting degree of electron accumulation, at the (001) and (111) [135]. In the photoemission spectra, finite spectral intensity can be observed close to the Fermi level in In 2 O 3 (see the magnified spectrum in Fig.…”
Section: Surface Conductivitymentioning
confidence: 77%
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