Evidence for carrier compensation by gallium vacancies during annealing of highly Si-doped β-Ga2O3

  • Katie R. Gann
  • , Naomi A. Pieczulewski
  • , Cameron A. Gorsak
  • , Joshua T. Buontempo
  • , Brenton A. Noesges
  • , Thaddeus Asel
  • , Daniel M. Dryden
  • , Hari P. Nair
  • , David A. Mueller
  • , Michael O. Thompson

Research output: Contribution to journalArticlepeer-review

Abstract

Net carrier densities in highly Si-doped β-Ga2O3 decrease during thermal annealing as a function of temperature, time, and PO2 for both in situ and implant-doped films. The mechanism for this loss has been attributed to the formation of gallium vacancies (VGa3−), which act as compensating acceptors and form passivating defect complexes. Samples doped above 3 × 1019 cm−3, annealed at the same temperature and PO2, ultimately approach a similar net carrier density of 1-3 × 1019 cm−3 (for 950 °C and PO2 < 2 × 10−7 bar) independent of the starting dopant concentration or doping method. These highly doped samples, metastable under these conditions, generate VGa3− to reach the steady state |ND − NA|, determined by the Fermi level. An activation energy of 1.6 ± 0.2 eV was observed for the rate of net carrier loss in high concentration in situ doped films. Scanning transmission electron microscopy and electrical results for implanted samples show that dopant activation, lattice recovery, and compensation are all active within the first minutes of annealing. Understanding the metastability of higher doping levels and VGa3− formation allows for the development of mitigation strategies to achieve highly Si-doped β-Ga2O3 by implant (8 × 1019 cm−3 with >70 cm2/V s mobility), including using the minimum required anneal time to achieve lattice recovery and dopant activation, reducing vacancy formation. Compensation initially limited full activation of deeper implants to 1 × 1020 cm−3; by protecting the free surface with a SiO2 cap during annealing, the activation efficiency doubled, and the mobility increased by 30%, highlighting the importance of controlling VGa3− formation and compensation.

Original languageEnglish
Article number115302
JournalJournal of Applied Physics
Volume138
Issue number11
DOIs
StatePublished - Sep 21 2025
Externally publishedYes

Funding

This research was supported by the Air Force Research Laboratory-Cornell Center for Epitaxial Solutions (ACCESS) under Grant No. FA9550-18-1-0529. The authors also acknowledge the use of the Cornell Center for Materials Research Shared Facilities supported through the NSF MRSEC program (DMR-1719875) and the Cornell NanoScale Facility, a member of the National Nanotechnology Coordinated Infrastructure (NNCI), which is supported by the National Science Foundation (Grant No. NNCI-2025233). C.A.G. acknowledges support from the National Defense Science and Engineering Graduate (NDSEG) fellowship.

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