MXene-GaAs heterojunctions: interface modeling, electronic properties and optical absorption

异质结 材料科学 肖特基势垒 费米能级 凝聚态物理 密度泛函理论 光电子学 电子 纳米技术 化学 计算化学 物理 量子力学 二极管
作者
Shuaiqi Zhou
出处
期刊:Materials research express [IOP Publishing]
卷期号:10 (12): 125003-125003 被引量:3
标识
DOI:10.1088/2053-1591/ad1356
摘要

Abstract MXene has gained favor in the field of material research and development due to its excellent two-dimensional structural properties, electronic structure properties, scalability, etc The heterostructures with MXene on one end not only make full use of the characteristics of MXene itself but also have the potential for transformative and application-rich materials when combined with other materials on the opposite end. Inspired by potentials in MXene-contained heterojunctions, this study focuses on the MXene-GaAs heterostructures to better understand their binding characters, structure features, and electron structures. First, the heterostructures (GaAs-Ti 3 C 2 O, GaAs-Ti 3 C 2 F, and GaAs-Ti 3 C 2 OH) are modeled aiming to provide comprehensive insights into their formation. The results reveal that the MXene layer in these heterostructures plays a crucial role in protecting the GaAs crystal, as evidenced by the substantial binding energy observed. Among the three heterostructures, GaAs-Ti 3 C 2 OH shows the closest proximity at the interface, attributed to the strong binding between MXene surfaces and Ga atoms. Various analyses, including binding energy calculations, charge polarization evaluations, interface electrostatic potential biases, and electron localization function studies, yield valuable insights into the formation process of these heterojunctions. Moreover, the incorporation of MXene layers enables electron conduction, effectively transforming the heterostructures into Schottky barriers. The density of states (DOS) analysis reveals pronounced peaks near the Fermi levels, indicating excellent electron mobility. Notably, all three heterostructures demonstrate weak magnetic features of the surface GaAs near the Fermi levels, imparted by the MXene layers. Lastly, optical simulations predict an absorption peak located around 4.3 eV for GaAs-Ti 3 C 2 OH.
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