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Band Alignment of the CdS/Cu2Zn(Sn1–xGex)Se4 Heterointerface and Electronic Properties at the Cu2Zn(Sn1–xGex)Se4 Surface: x = 0, 0.2, and 0.4

覆盖层 材料科学 X射线光电子能谱 带材弯曲 异质结 费米能级 带偏移量 带隙 电子结构 分析化学(期刊) 电子能带结构 凝聚态物理 光电子学 价带 化学 电子 核磁共振 物理 量子力学 色谱法
作者
Takehiko Nagai,Takuya Shimamura,Kohei Tanigawa,Yuya Iwamoto,Hiroya Hamada,Nobuyoshi Ohta,Shinho Kim,Hitoshi Tampo,Hajime Shibata,Koji Matsubara,Shigeru Niki,Norio Terada
出处
期刊:ACS Applied Materials & Interfaces [American Chemical Society]
卷期号:11 (4): 4637-4648 被引量:32
标识
DOI:10.1021/acsami.8b19200
摘要

The surface electronic properties of the light absorber and band alignment at the p/n heterointerface are key issues for high-performance heterojunction solar cells. We investigated the band alignment of the heterointerface between cadmium sulfide (CdS) and Ge-incorporated Cu2ZnSnSe4 (CZTGSe), with Ge/(Ge + Sn) ratios (x) between 0 and 0.4, by X-ray photoelectron, ultraviolet, and inversed photoemission spectroscopies (XPS, UPS, and IPES, respectively). In particular, we used interface-induced band bending in order to determine the conduction band offset (CBO) and valence-band offset (VBO), which were calculated from the core-level shifts of each element in both the CdS overlayer and the CZTGSe bottom layer. Moreover, the surface electronic properties of CZTGSe were also investigated by laser-irradiated XPS. The CBO at the CdS/CZTGSe heterointerface decreased linearly, from +0.36 to +0.20 eV, as x was increased from 0 to 0.4; in contrast, the VBO at the CdS/CZTGSe heterointerface was independent of Ge content. Both UPS and IPES revealed that the Fermi level at the CZTGSe surface is located near the center of the band gap. The hole concentration at the CZTGSe surface was on the order of 1011 cm–3, which is much smaller than that of the bulk (∼1016 cm–3). We discuss the differences in hole deficiencies near the surface and in the bulk on the basis of laser-irradiated XPS and conclude that hole deficiencies are due to defects distributed near the surface with densities that are lower than in the bulk, and the Fermi level is not pinned at the CZTGSe surface.
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