SrHfO3 is a potential dielectric material for metal-oxide-semiconductor devices. The SrHfO3/GaAs interface has attracted attention because of its unique properties. In this paper, the interface properties of (001) SrHfO3/GaAs are investigated by first-principles calculations based on density functional theory. First, the adsorption behavior of Sr, Hf, and O atoms on the GaAs surface is investigated. An O atom has a lower adsorption energy on a Ga surface than on an As surface. Then, some possible (001) SrHfO3/GaAs configurations are considered to analyze the interface spacing, stability, band offsets, and charge transfer. The SrO/Ga(1) and HfO2/Ga(2) configurations are lower in binding energy than other interface configurations, indicating that they are more stable. Finally, we study the electronic properties of the SrO/Ga(1) and HfO2/Ga(2) configurations. The electronic density of states suggests that these systems exhibit metallic behavior. The band offset and charge transfer are related to the interface spacing. The valence band offset and charge transfer decrease with increasing interface spacing. Published by AIP Publishing.
机构:
State Key Laboratory of Gansu Advanced Non-ferrous Metal Materials,Department of Materials Science and Engineering,Lanzhou University of Technology
Science and Technology on Surface Engineering Laboratory Lanzhou Institute of PhysicsState Key Laboratory of Gansu Advanced Non-ferrous Metal Materials,Department of Materials Science and Engineering,Lanzhou University of Technology
刘冉
薛红涛
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State Key Laboratory of Gansu Advanced Non-ferrous Metal Materials,Department of Materials Science and Engineering,Lanzhou University of TechnologyState Key Laboratory of Gansu Advanced Non-ferrous Metal Materials,Department of Materials Science and Engineering,Lanzhou University of Technology
薛红涛
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路文江
冯煜东
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Science and Technology on Surface Engineering Laboratory Lanzhou Institute of PhysicsState Key Laboratory of Gansu Advanced Non-ferrous Metal Materials,Department of Materials Science and Engineering,Lanzhou University of Technology
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Lanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China
Lanzhou Inst Phys, Sci & Technol Surface Engn Lab, Lanzhou 730000, Peoples R ChinaLanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China
Tang Fu-Ling
Liu Ran
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Lanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China
Lanzhou Inst Phys, Sci & Technol Surface Engn Lab, Lanzhou 730000, Peoples R ChinaLanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China
Liu Ran
Xue Hong-Tao
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Lanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R ChinaLanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China
Xue Hong-Tao
Lu Wen-Jiang
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Lanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R ChinaLanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China
Lu Wen-Jiang
Feng Yu-Dong
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Lanzhou Inst Phys, Sci & Technol Surface Engn Lab, Lanzhou 730000, Peoples R ChinaLanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China
Feng Yu-Dong
Rui Zhi-Yuan
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Lanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R ChinaLanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China
Rui Zhi-Yuan
Huang Min
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Chinese Acad Sci, Wuhan Inst Phys & Math, State Key Lab Magnet Resonance & Atom & Mol Phys, Wuhan 430071, Peoples R ChinaLanzhou Univ Technol, Dept Mat Sci & Engn, State Key Lab Gansu Adv Nonferrous Met Mat, Lanzhou 730050, Peoples R China