Limitations on activation of high dose Ge implants in <i>β</i> -Ga2O3

T Tianhai Luo (Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,) K Katie R. Gann (Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,) C Cameron A. Gorsak (Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,) M Ming-Chiang Chang (Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,) P Prescott E. Evans (Air Force Research Laboratory 2 , Wright-Patterson AFB, Dayton, Ohio 45433,) T Thaddeus J. Asel H Hari P. Nair (Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,) R R. B. van Dover (Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,) M Michael O. Thompson (Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,)

Abstract

Among ultrawide bandgap semiconductors, β-Ga2O3 is particularly promising for high power and frequency applications. For devices, n-type concentrations above 1019 cm−3 are required. Ge is a promising alternative n-type dopant with an ionic radius similar to Ga. Homoepitaxial (010) β-Ga2O3 films were implanted with Ge to form 50 and 100 nm box concentrations of 3 × 1019 and 5 × 1019 cm−3, with damage ranging from 1.2 to 2.0 displacements per atom. For lower damage implants, optimized anneals in ultrahigh purity N2 at 950–1000 °C for 5–10 min resulted in an RS of 600–700 Ω/□, mobilities of 60–70 cm2/V s, and a Ge activation of up to 40%. For higher damage implants, activation dropped to 23% with similar mobilities. Ge diffusion, measured by secondary ion mass spectrometry, showed the formation of a Ge “clustering peak” with a concentration exceeding the initial implant following anneals in N2 or O2 at 950–1050 °C. Beyond this peak, minimal Ge diffusion occurred for N2 anneals at 950 °C, but at 1050 °C, non-Fickian diffusion extended to &amp;gt;200 nm. Electrical activation data suggest that clustered Ge is electrically inactive. To understand Ge clustering, several samples were characterized by synchrotron x-ray diffraction. Second-phase precipitates were observed in as-implanted samples, which then fully dissolved after furnace annealing in N2 at 1050 °C. Diffraction peaks suggest that these implant-induced precipitates may be related to a high pressure Pa3¯ phase of GeO2 and may evolve during anneals to explain the Ge clustering. Ultimately, we believe that Ge clustering limits the activation of implanted Ge at high concentrations.

Article Details

Volume / Issue Vol. 139, Issue 9
Published March 07, 2026
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (9)

T

Tianhai Luo

Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,

K

Katie R. Gann

Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,

C

Cameron A. Gorsak

Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,

M

Ming-Chiang Chang

Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,

P

Prescott E. Evans

Air Force Research Laboratory 2 , Wright-Patterson AFB, Dayton, Ohio 45433,

T

Thaddeus J. Asel

H

Hari P. Nair

Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,

R

R. B. van Dover

Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,

M

Michael O. Thompson

Department of Materials Science and Engineering, Cornell University 1 , Ithaca, New York 14853,