April 22 - 26, 2024
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May 7 - 9, 2024 (Virtual)
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EL04.09.03

MBE Growth and Properties of Monoclinic (AlxGa1-x-yIny)2O3 Alloys

When and Where

Apr 25, 2024
9:00am - 9:15am
Room 345, Level 3, Summit

Presenter(s)

Co-Author(s)

Marshall Tellekamp1,Stephen Schaefer1,Kingsley Egbo1,Glenn Teeter1,Syed Hasan1,Andriy Zakutayev1

National Renewable Energy Laboratory1

Abstract

Marshall Tellekamp1,Stephen Schaefer1,Kingsley Egbo1,Glenn Teeter1,Syed Hasan1,Andriy Zakutayev1

National Renewable Energy Laboratory1
Gallium oxide (Ga<sub>2</sub>O<sub>3</sub>) is an emerging ultra-wide bandgap semiconductor material that has attracted attention for its potential to outperform existing SiC and GaN based devices operating at high breakdown voltages and high temperature. The thermodynamically stable phase at room temperature and pressure is the monoclinic β-phase with symmetry <i>C2/m</i>. β-Ga<sub>2</sub>O<sub>3</sub> has a direct bandgap energy of 4.76 eV and critical field as high as 8 MV/cm. Isovalent alloying of In and Al in β-Ga<sub>2</sub>O<sub>3</sub> provides the ability to engineer bandgap energy and strain of the material, however the monoclinic structure is not the ground state for Al<sub>2</sub>O<sub>3</sub> or In<sub>2</sub>O<sub>3</sub>. First-principles calculations indicate a range of bandgap energies from 7.2-7.5 eV for monoclinic θ-Al<sub>2</sub>O<sub>3</sub> to 2.7 eV for monoclinic In<sub>2</sub>O<sub>3</sub>. The corresponding lattice mismatch to β-Ga<sub>2</sub>O<sub>3</sub> ranges from about 4% for θ-Al<sub>2</sub>O<sub>3</sub> to 10% for monoclinic In<sub>2</sub>O<sub>3</sub>. In principle the quaternary (Al<sub>x</sub>Ga<sub>1-x-y</sub>In<sub>y</sub>)<sub>2</sub>O<sub>3</sub> can span this bandgap energy and strain range, providing device designers with additional degrees of freedom to tune band offsets and electronic properties.<br/><br/>However, efforts to synthesize isovalent alloys are complicated by their tendency to phase separate. Strain balanced alloys of (Al<sub>x</sub>Ga<sub>1-x</sub>)<sub>2</sub>O<sub>3 </sub>and (In<sub>x</sub>Ga<sub>1-x</sub>)<sub>2</sub>O<sub>3</sub> may be able to overcome the tendency for phase separation and stabilize the monoclinic crystal, however literature reports of the quaternary (Al<sub>x</sub>Ga<sub>1-x-y</sub>In<sub>y</sub>)<sub>2</sub>O<sub>3 </sub>are limited to &lt;1% unintentional indium incorporation in In-catalyzed (Al<sub>x</sub>Ga<sub>1-x</sub>)<sub>2</sub>O<sub>3</sub>.<sup>1</sup> The primary limitation to quaternary formation is the limited incorporation of indium at elevated growth temperatures. This limited incorporation is due to both the volatility of indium oxide and Al and Ga cation exchange reactions which replace indium in In<sub>2</sub>O<sub>3</sub>.<sup>2</sup><br/><br/>We report on the first successful synthesis of phase pure monoclinic (Al<sub>x</sub>Ga<sub>1-x-y</sub>In<sub>y</sub>)<sub>2</sub>O<sub>3</sub> by molecular beam epitaxy. Plasma-assisted molecular beam epitaxy (MBE) is used to grow (Al<sub>x</sub>Ga<sub>1-x-y</sub>In<sub>y</sub>)<sub>2</sub>O<sub>3</sub> on (010) oriented Fe doped β-Ga<sub>2</sub>O<sub>3</sub> substrates at 750 °C and Ga and In beam equivalent pressures (BEP) of 5×10<sup>-8</sup> and 2×10<sup>-7</sup> torr, respectively. The Al BEP varies from 1×10<sup>-9</sup> to 1.5×10<sup>-8</sup> torr. X-ray diffraction measurements of the (020) plane indicate a strained film consistent with the structural incorporation of both Al and In, and this incorporation is chemically corroborated by x-ray fluorescence (XRF) and X-ray photoemission spectroscopy (XPS). Wide-angle ω-2θ survey scans confirm the absence of additional XRD peaks, indicating the films are monoclinic with no phase separation. Spectroscopic ellipsometry measurements show a monotonic shift in the extinction coefficient edge from approximately 4.7 to 5.2 eV with increasing Al BEP. Additional structural, chemical, optical, and electrical characterization measurements including Rutherford back-scattering spectrometry, scanning tunneling microscopy will be presented, concluding with an outlook on the applicability of these quaternary films to gallium oxide device design.<br/><br/>[1] P. Vogt, A. Mauze, F. Wu, B. Bonef, and J. S. Speck, "Metal-oxide catalyzed epitaxy (MOCATAXY): the example of the O plasma-assisted molecular beam epitaxy of β-(Al<sub>x</sub>Ga<sub>1-x</sub>)<sub>2</sub>O<sub>3</sub>/β-Ga<sub>2</sub>O<sub>3</sub> heterostructures", Appl. Phys. Express <b>11</b>, 115503 (2018).<br/>[2] P. Vogt, O. Brandt, H. Riechert, J. Lähnemann, and O. Bierwagen, "Metal-Exchange Catalysis in the Growth of Sesquioxides: Towards Heterostructures of Transparent Oxide Semiconductors", Phys. Rev. Lett. <b>119</b>, 196001 (2017).

Keywords

alloy | molecular beam epitaxy (MBE) | oxide

Symposium Organizers

Hideki Hirayama, RIKEN
Robert Kaplar, Sandia National Laboratories
Sriram Krishnamoorthy, University of California, Santa Barbara
Matteo Meneghini, University of Padova

Symposium Support

Silver
Taiyo Nippon Sanso

Session Chairs

Sriram Krishnamoorthy
Joel Varley

In this Session