Reexamination of band offset transitivity employing oxide heterojunctions
Xiaolei Wang, Jinjuan Xiang, Wenwu Wang, Jing Zhang, Kai Han, Hong Yang, Xueli Ma, Chao Zhao, Dapeng Chen, Tianchun Ye
Abstract
Xiaolei Wang, Jinjuan Xiang, Wenwu Wang, Jing Zhang, Kai Han, Hong Yang, Xueli Ma, Chao Zhao, Dapeng Chen, Tianchun Ye
Abstract
Band offset transitivity is reexamined extendedly by employing oxide heterojuctions. The valence band offsets (ΔEV) at HfO2/SiO2, Al2O3/SiO2, and HfO2/Al2O3 heterojunctions are experimentally determined to be 0.81, 0.25, and 0.25 eV, respectively, by X-ray photoelectron spectroscopy. Thus, the ΔEV at HfO2/Al2O3 heterojunction is not equal to the ΔEV at HfO2/SiO2 minus the ΔEV at Al2O3/SiO2 heterostructures (0.25 ≠ 0.81 − 0.25 = 0.56), i.e., the transitivity rule fails for oxide heterojunctions. Different distributions of interfacial induced gap states at the three heterostructures contribute to this failure of transitivity rule.
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Band offset transitivity is reexamined extendedly by employing oxide heterojuctions. The valence band offsets (ΔEV) at HfO2/SiO2, Al2O3/SiO2, and HfO2/Al2O3 heterojunctions are experimentally determined to be 0.81, 0.25, and 0.25 eV, respectively, by X-ray photoelectron spectroscopy. Thus, the ΔEV at HfO2/Al2O3 heterojunction is not equal to the ΔEV at HfO2/SiO2 minus the ΔEV at Al2O3/SiO2 heterostructures (0.25 ≠ 0.81 − 0.25 = 0.56), i.e., the transitivity rule fails for oxide heterojunctions. Different distributions of interfacial induced gap states at the three heterostructures contribute to this failure of transitivity rule.
Key concepts: Heterojunction, Valence band, X-ray photoelectron spectroscopy, Band offset, Oxide, Offset (computer science), Transitive relation, Band diagram