Growth of conductive Si-doped α-Ga2O3 by suboxide molecular-beam epitaxy

Jacob Steele, Julianne Chen, Tamá Burrell, Naomi A. Pieczulewski, Debaditya Bhattacharya, Kathleen Smith, Katie Gann, Michael O. Thompson, Huili G. Xing, Debdeep Jena, David A. Muller, Michael D. Williams, M. K.Indika Senevirathna, Darrell G. Schlom

Research output: Contribution to journalArticlepeer-review

Abstract

We report a two-step film-growth process using suboxide molecular-beam epitaxy (S-MBE) that produces Si-doped α-Ga2O3 with record transport properties. The method involves growing a relaxed α-(AlxGa1−x)2O3 buffer layer on m-plane sapphire at a relatively high substrate temperature (Tsub), ∼750 °C, followed by an Si-doped α-Ga2O3 overlayer grown at lower Tsub, ∼500 °C. The high Tsub allows the ∼3.6% lattice-mismatched α-(AlxGa1−x)2O3 buffer with x = 0.08 ± 0.02 to remain epitaxial and phase pure during relaxation to form a pseudosubstrate for the overgrowth of α-Ga2O3. The optimal conditions for the subsequent growth of Si-doped α-Ga2O3 by S-MBE are 425 °C ≤ Tsub ≤ 500 °C and P80% O3 = 5 × 10−6 Torr. Si-doped α-Ga2O3 films grown with this method at Tsub > 550 °C are always insulating. Secondary-ion mass spectrometry confirms that both the insulating and conductive films have uniform silicon incorporation. In conductive films with 1019 ≤ NSi ≤ 1020 cm−3, the incorporated silicon is ∼100% electrically active. At NSi ≤ 1019 cm−3, the carrier concentration (n) plummets. A maximum Hall mobility (μ) = 90 cm 2 V·s at room-temperature is measured in a film with n = 2.9 × 1019 cm−3 and a maximum conductivity (σ) = 650 S/cm at room-temperature in a film with n = 4.8 × 1019 cm−3. A threading dislocation density of (5.6 ± 0.6) × 1010 cm−2 is revealed by scanning transmission electron microscopy, showing that there is still enormous room to improve the electrical properties of doped α-Ga2O3 thin films.

Original languageEnglish
Article number101117
JournalAPL Materials
Volume13
Issue number10
DOIs
StatePublished - Oct 1 2025
Externally publishedYes

Funding

This work was primarily supported by the AFOSR/AFRL ACCESS Center of Excellence under Award No. FA9550-18-1-0529. This work was supported in part by SUPREME, one of seven centers supported by the Semiconductor Research Corporation (SRC) and DARPA under the Joint University Microelectronics Program 2.0 (JUMP 2.0). This work made use of the Cornell Energy Systems Institute Shared Facilities, partly sponsored by the NSF (Grant No. MRI DMR-1631282). The STEM work also made use of the electron microscopy facility of the Cornell Center for Materials Research (CCMR) with support from the National Science Foundation Materials Research Science and Engineering Centers (MRSEC) program (Grant No. DMR-1719875). N.A.P. acknowledges support from the National Science Foundation Graduate Research Fellowship under Grant No. DGE2139899. The Thermo Fisher Spectra 300 X-CFEG was acquired with support from PARADIM, an NSF MIP (Grant No. DMR-2039380), and Cornell University. M.K.I.S., M.D.W., and D.G.S. acknowledge additional funding from Grant No. NSF-PREM-DMR-2122147.

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