Castellanos-Águila Jesús Eduardo, Palacios Clemente Pablo, García Gregorio, Olea-Amezcua Mónica Araceli, Rivas-Silva Juan Francisco, Wahnón Perla
Departamento de Estudios Multidisciplinarios, Universidad de Guanajuato, Av. Yacatitas, S/N Col. Yacatitas, Yuriria, Guanajuato C.P. 36940, México.
Instituto de Energía Solar, Universidad Politécnica de Madrid, 28040 Madrid, Spain.
ACS Omega. 2020 Feb 13;5(7):3294-3301. doi: 10.1021/acsomega.9b03362. eCollection 2020 Feb 25.
The valence and conduction band offsets for both polar and nonpolar CuGaS/CuAlSe and CuGaS/ZnSe interfaces were studied here by the state-of-the-art first-principles calculations. Using the hybrid functional calculations, we show that the CuGaS/CuAlSe and CuGaS/ZnSe heterostructures in all interfaces form type II band alignment. The difference of valence and conduction band offsets is mainly due to lattice mismatch, generating stress in the interface and affecting the electronic properties of each material; meanwhile, the polarity configuration does not play an important role in these values. From the local density of states and the charge density, we can determine how the nature of the band alignments changes when the semiconductor conforms to each interface. This allows us to localize the electrons and holes at different sites of the interface.
本文通过最先进的第一性原理计算研究了极性和非极性CuGaS/CuAlSe以及CuGaS/ZnSe界面的价带和导带偏移。使用杂化泛函计算,我们表明所有界面处的CuGaS/CuAlSe和CuGaS/ZnSe异质结构均形成II型能带排列。价带和导带偏移的差异主要归因于晶格失配,在界面处产生应力并影响每种材料的电子性质;同时,极性配置在这些值中并不起重要作用。从局域态密度和电荷密度,我们可以确定当半导体与每个界面符合时能带排列的性质如何变化。这使我们能够将电子和空穴定位在界面的不同位置。