Optical and electronic properties of (InxGa1−x)2O3 alloys

B Bishal Shrestha (Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,) M Madan K. Mainali (Department of Physics and Astronomy &Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,) P Prabin Dulal (Department of Physics and Astronomy &Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,) M Manoj K. Jamarkattel (Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,) A Abdul Quader (Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,) E Ebin Bastola (Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,) A Adam B. Phillips (Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,) M Michael J. Heben (Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,) N Nikolas J. Podraza (Department of Physics and Astronomy &Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,)

Abstract

Indium gallium oxide [(InxGa1−x)2O3] alloys are of interest for a variety opto-electronic applications including photovoltaic devices owing to the ability to control properties through alloy composition. A thorough evaluation of the opto-electronic properties of (InxGa1−x)2O3 (x = 0.71, 0.55, 0.45, 0.36, and 0.28) thin films is obtained by using terahertz to ultraviolet range spectroscopic ellipsometry to measure the complex dielectric function (ɛ = ɛ1 + iɛ2) spectra from 0.400 meV to 5.877 eV and the derived vibrational modes from chemical bonding, inter-band transition energies, and carrier transport properties. Optical band edges of direct and non-direct transitions increase from 3.82 to 4.14 eV and 2.96 to 3.36 eV, respectively, with decreasing In-content, whereas the carrier concentration determined from the direct electrical Hall effect and spectroscopic ellipsometry measurements decreases from ∼1020 to 1018 cm−3. Mobilities (μSE), resistivities (ρSE), and carrier effective masses (m*SE) from the spectroscopic ellipsometry range from ∼10.6 to ∼66.8 cm2 V−1 s−1, 2.3 × 10−3, to 47.1 × 10−3 Ω cm, and 0.308 to 0.397 me, respectively. μSE and ρSE are compared to those obtained from the direct electrical Hall effect and four-point probe measurements with discrepancies attributed to principles of measurement techniques. Spectroscopic ellipsometry determined parameters are representative of properties within localized regions, whereas direct electrical measurements are influenced by a greater degree of charge carrier scattering due to longer path lengths of travel.

Article Details

Volume / Issue Vol. 137, Issue 3
Published January 21, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (9)

B

Bishal Shrestha

Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,

M

Madan K. Mainali

Department of Physics and Astronomy &Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,

P

Prabin Dulal

Department of Physics and Astronomy &Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,

M

Manoj K. Jamarkattel

Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,

A

Abdul Quader

Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,

E

Ebin Bastola

Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,

A

Adam B. Phillips

Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,

M

Michael J. Heben

Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,

N

Nikolas J. Podraza

Department of Physics and Astronomy &Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo , Toledo, Ohio 43606,