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Fizika i Tekhnika Poluprovodnikov, 2024 Volume 58, Issue 9, Pages 513–523 (Mi phts6792)

Surface, interfaces, thin films

Modification of near-surface layers of alpha-gallium oxide under irradiation with ultra-high ion doses

E. D. Fedorenkoa, A. I. Klevtsova, A. I. Titova, V. D. Andreevaa, A. L. Shakhmina, P. A. Karaseova, A. I. Pechnikovb, V. I. Nikolaevb

a Peter the Great St. Petersburg Polytechnic University, 195251 St. Petersburg, Russia
b Ioffe Institute, 194021 St. Petersburg, Russia

Abstract: A detailed study of $\alpha$-Ga$_2$O$_3$ epitaxial layers grown by halide vapor phase epitaxy has been carried out both before and after P and Ta and molecular PF$_4$ ion bombardment to doses as high as 45 dpa. A wide range of complementary analytical techniques were used: X-ray diffraction, atomic force microscopy, Rutherford backscattering spectrometry in channeling mode and X-ray photoelectron spectroscopy. Completely amorphous layer is formed from the surface to the crystal bulk as a result of irradiation. Monatomic P and Ta ions form thicker amorphous layer than molecular PF$_4$ ions. Small step appears at the border between virgin and irradiated areas of the sample revealing sample swelling ($\sim$7 nm after irradiation to 45 dpa). The root mean square roughness of the $\alpha$-Ga$_2$O$_3$ surface remains approximately unchanged (0.7 to 0.5 nm) after irradiation to a dose up to 45 dpa, regardless of the ion kind. The smoothing of small-scale topography (reflecting atomic steps) due to irradiation-induced amorphization of the sub-surface layer is found, whereas the large-scale topography remains virtually unchanged. Ion bombardment leads to surface layer decomposition with oxygen loss and partial reduction of gallium to Ga$^0$ and Ga$^+$ states.

Keywords: gallium oxide, $\alpha$-Ga$_2$O$_3$, ion bombardment, high-dose irradiation, modification of sub-surface layers, ion radiation effects, surface topography, structural defects, X-ray photoelectron spectroscopy, AFM.

Received: 03.10.2024
Revised: 29.10.2024
Accepted: 11.11.2024

DOI: 10.61011/FTP.2024.09.59313.7126



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© Steklov Math. Inst. of RAS, 2025