Galazka, Zbigniew, Ganschow, Steffen, Irmscher, Klaus, Klimm, Detlef, Albrecht, Martin, Schewski, Robert, Pietsch, Mike, Schulz, Tobias, Dittmar, Andrea, Kwasniewski, Albert, Grueneberg, Raimund, Anooz, Saud Bin, Popp, Andreas, Juda, Uta, Hanke, Isabelle M., Schroeder, Thomas, and Bickermann, Matthias
In the course of development of transparent semiconducting oxides (TSOs) we compare the growth and basic physical properties bulk single crystals of ultra-wide bandgap (UWBG) TSOs, namely β-Ga 2 O 3 and Ga-based spinels MgGa 2 O 4 , ZnGa 2 O 4 , and Zn 1-x Mg x Ga 2 O 4. High melting points of the materials of about 1800 -1930 °C and their thermal instability, including incongruent decomposition of Ga-based spinels, require additional tools to obtain large crystal volume of high structural quality that can be used for electronic and optoelectronic devices. Bulk β-Ga 2 O 3 single crystals were grown by the Czochralski method with a diameter up to 2 inch, while the Ga-based spinel single crystals either by the Czochralski, Kyropoulos-like, or vertical gradient freeze / Bridgman methods with a volume of several to over a dozen cm3. The UWBG TSOs discussed here have optical bandgaps of about 4.6 - 5 eV and great transparency in the UV / visible spectrum. The materials can be obtained as electrical insulators, n -type semiconductors, or n -type degenerate semiconductors. The free electron concentration (n e) of bulk β-Ga 2 O 3 crystals can be tuned within three orders of magnitude 1016 - 1019 cm−3 with a maximum Hall electron mobility (μ) of 160 cm2V−1s−1, that gradually decreases with n e. In the case of the bulk Ga-based spinel crystals with no intentional doping, the maximum of n e and μ increase with decreasing the Mg content in the compound and reach values of about 1020 cm−3 and about 100 cm2V−1s−1 (at n e > 1019 cm−3), respectively, for pure ZnGa 2 O 4. [ABSTRACT FROM AUTHOR]