Epitaxial <inline-formula> <tex-math notation="LaTeX">$\beta$ </tex-math> </inline-formula>-Ga<sub>2</sub>O<sub>3</sub> and <inline-formula> <tex-math notation="LaTeX">$\beta$ </tex-math> </inline-formula>-(Al<sub>x</sub>Ga<sub>1−x</sub>)<sub>2</sub>O<sub>3</sub>/<inline-formula> <tex-math notation="LaTeX">$\beta$ </tex-math> </inline-formula>-Ga<sub>2</sub>O<sub>3</sub> Heterostructures Growth for Power Electronics (2018)

We report on the growth of high quality β-Ga <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> films using metal organic chemical vapor deposition (MOCVD). Ga(DPM) <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> , TEGa, and TMGa metal organic precursors were used as Ga sources and oxygen for oxidation. Films grown from each Ga sources had high growth rates with up to 10 μm/h achieved using TMGa. To study the quality homoepitaxial layers, MOCVD was used to grow unintentionally doped (UID) and Si doped β-Ga <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> layers with a growth rate between 0.5 and 4.0 μm/h Epitaxial layers with XRD FWHM and RMS roughness <; 50 arcsec and <; 0.5 nm, respectively, were demonstrated. The electron mobility increased from ~13 cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> /Vs for n = 8×10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">19</sup> 1/cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sup> to ~120 cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> /Vs for n = 1.6×10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">17</sup> 1/cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sup> . These values are comparable with the best literature data, despite higher growth rates. For the UID β-Ga <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> layers, Si was identified as the major impurity responsible for the free carrier concentration with strong accumulation at the film/substrate interface. The reactor was also used to grow high quality strained β-(Al <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> Ga <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1-x</sub> ) <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> /β-Ga <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> heterostructures and superlattices with Al content of up to 43%. The results suggest that the MOCVD enables growth of device quality β-Ga <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> and related alloys at a fast growth rate which is critical for high voltage power devices.