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    Determining the band alignment at the (010)-oriented β-(AlxGa1−x)2O3/Ga2O3 interface using hard x-ray photoemission spectroscopy and ab initio calculations

    Wenjing Xu1,2, Hailing Guo3, Zhenni Yang2, Yihong Chen1,2, Xiangyu Xu1, Tien-Lin Lee4, Duanyang Chen2,5, Xinxin Yu6,7, Yuzheng Guo3 et al.

    Zhaofu Zhang8,*, Hongji Qi2,5,†, and Kelvin H.L. Zhang1,‡

    • *Contact author: zhaofuzhang@whu.edu.cn
    • †Contact author: qhj@siom.ac.cn
    • ‡Contact author: kelvinzhang@xmu.edu.cn

    Phys. Rev. Applied 24, 044016 – Published 6 October, 2025

    DOI: https://doi.org/10.1103/255q-v9k4

    Abstract

    In this work, we investigate the electronic structure and interfacial band alignment of β-(AlxGa1−x)2O3/Ga2O3 heterojunctions using a combination of synchrotron-based hard x-ray photoemission spectroscopy (HAXPES) and first-principles hybrid density functional theory calculations. β-(AlxGa1−x)2O3 films with Al compositions of x = 0.12, 0.19, and 0.29 were grown on Fe-doped β-Ga2O3 (010) substrates via pulsed laser deposition. The band gap of β-(AlxGa1−x)2O3 increases from (4.83 ± 0.05) eV (x = 0) to (5.37 ± 0.08) eV (x = 0.29), primarily driven by an upward shift of the conduction band edge due to hybridization between Al 3s and Ga 4s states, while the valence band edge exhibits a slight downward shift. Both experimental HAXPES data and theoretical calculations confirmed the formation of a “type I” (straddling) band alignment in the β-(AlxGa1−x)2O3/Ga2O3 heterojunctions. For instance, at x = 0.29, the conduction band offset and valence band offset are approximately 0.33 and 0.21 eV, respectively. These findings provide valuable insights for designing modulation-doped β-(AlxGa1−x)2O3/Ga2O3 heterostructures, enabling the realization of a two-dimensional electron gas and its application in high-frequency electronic devices.

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