Stephan Lany1,Anuj Goyal1,Andriy Zakutayev1,Vladan Stevanovic2
National Renewable Energy Laboratory1,Colorado School of Mines2
Stephan Lany1,Anuj Goyal1,Andriy Zakutayev1,Vladan Stevanovic2
National Renewable Energy Laboratory1,Colorado School of Mines2
Ga<sub>2</sub>O<sub>3</sub> is being actively explored for optoelectronic (phosphorus, and electroluminescent devices, solar-blind photodetectors) applications due to its ultra-wide bandgap and low projected fabrication cost of large-size and high-quality crystals. Efficient <i>n</i>-type doping of Ga<sub>2</sub>O<sub>3</sub> has been achieved, but <i>p</i>-type doping faces fundamental obstacles due to compensation, deep acceptor levels, and the polaron transport mechanism of free holes. However, aside from achieving <i>p</i>-type conductivity, plenty of opportunity exists to engineer the position of the Fermi level for improved design of Ga<sub>2</sub>O<sub>3</sub> based devices. We use first-principles defect theory and defect equilibrium calculations to simulate a 3-step growth-annealing-quench synthesis protocol for hydrogen assisted Mg doping in β-Ga<sub>2</sub>O<sub>3</sub>, considering the gas phase equilibrium between H<sub>2</sub>, O<sub>2</sub> and H<sub>2</sub>O, which determines the H chemical potential. We predict Ga<sub>2</sub>O<sub>3</sub> doping-type conversion to a net <i>p</i>-type regime after growth under reducing conditions in the presence of H<sub>2 </sub>followed by O-rich annealing, which is a similar process to the Mg acceptor activation by H removal in GaN. We show that there is an optimal temperature that maximizes the Ga<sub>2</sub>O<sub>3</sub> net acceptor density for a given Mg doping level. After quenching to operating temperature, the Ga<sub>2</sub>O<sub>3</sub> Fermi level drops below mid-gap down to about +1.5 eV above the valence band maximum, creating a significant number of uncompensated neutral Mg<sub>Ga</sub><sup>0</sup> acceptors. The resulting free hole concentration in Ga<sub>2</sub>O<sub>3</sub> is very low due to deep energy level of these Mg acceptors, and hole conductivity is further impeded by the polaron hopping mechanism. However, the Fermi level reduction down to +1.5 eV and suppression of free electron density in this doping type converted (<i>N</i><sub>A</sub> > <i>N</i><sub>D</sub>) Ga<sub>2</sub>O<sub>3</sub> material is of significance and impact for the design of Ga<sub>2</sub>O<sub>3</sub> based optoelectronic devices.<br/>Reference: J. Appl. Phys. 129, 245704 (2021); https://doi.org/10.1063/5.0051788