MRS Meetings and Events

 

EQ01.01.04 2022 MRS Spring Meeting

Computational Fermi Level Engineering and Doping-Type Conversion of Ga2O3 via Three-Step Processing

When and Where

May 9, 2022
11:30am - 11:45am

Hawai'i Convention Center, Level 3, 318B

Presenter

Co-Author(s)

Stephan Lany1,Anuj Goyal1,Andriy Zakutayev1,Vladan Stevanovic2

National Renewable Energy Laboratory1,Colorado School of Mines2

Abstract

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> &gt; <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

Keywords

defects

Symposium Organizers

Robert Kaplar, Sandia National Laboratories
Srabanti Chowdhury, Stanford University
Yoshinao Kumagai, Tokyo University of Agriculture and Technology
Julien Pernot, University of Grenoble Alpes

Publishing Alliance

MRS publishes with Springer Nature