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Optical Properties of Indium-Gallium-Oxide Microcrystalline Alloy Films: From the Visible to the Deep-UV
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Optical Properties of Indium-Gallium-Oxide Microcrystalline Alloy Films: From the Visible to the Deep-UV

HM Borhanul Alam, Dipak Oli, You Qiang, Bisheswor Acharya, Jesse Huso, Matthew D McCluskey and Leah Bergman
arXiv
04/26/2026

Abstract

Physics - Materials Science
The tailored optical properties of(InₓGa₁₋ₓ)₂O₃microcrystalline films were studied as a function of composition x via transmission, Urbach energy analysis, and spatial photoluminescence (PL) mapping of the self-trapped hole (STH) emission, with the objective of addressing material characteristics specific to this alloy system. Up to x = 0.46, the optical gap exhibited a redshift of 1 eV from the deep to the near-UV range, while the STH PL was redshifted by 0.5 eV in the visible range. For higher composition, x = 0.63, the transmission spectra indicated the co-existence of two optical gaps attributed to Ga-rich and to In-rich domains, implying that this sample is phase-separated. However, the saturation behavior of the optical gap and that of the STH PL showed that incipient phase separation occurs at a lower composition: x 0.3. This is consistent with the compositional trend found for Urbach energy, implying that phase segregation in the alloys is a major defect even at its incipient stages. Additionally, Urbach analysis of(InₓGa₁₋ₓ)₂O₃was compared to that ofMgₓZn₁₋ₓO . Both systems were found to have similar compositional dependence: at lower range, Urbach energies exhibited a negligible increase, while at the higher range a significant dependence on the composition was found. The main difference between the two alloy systems is in their Urbach energy: those for(InₓGa₁₋ₓ)₂O₃were significantly larger than those ofMgₓZn₁₋ₓO . This stems from the strong hole coupling to phonons of(InₓGa₁₋ₓ)₂O₃ , which provides a dynamic transition additionally to that of defect-type.
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