锌黄锡矿
X射线光电子能谱
化学浴沉积
量子效率
溅射
带隙
薄膜
材料科学
分析化学(期刊)
图层(电子)
开路电压
沉积(地质)
太阳能电池
光电子学
化学
化学工程
纳米技术
捷克先令
电压
古生物学
物理
色谱法
量子力学
沉积物
工程类
生物
作者
Willi Kogler,Thomas Schnabel,Erik Ahlswede,Teoman Taskesen,Levent Gütay,Dirk Hauschild,L. Weinhardt,Clemens Heske,Jasmin Seeger,M. Hetterich,Michael Powalla
摘要
To replace the conventionally used CdS buffers in Cu2ZnSn(S,Se)4 (CZTSSe) based thin-film solar cells, sputtered Zn(O,S) buffer layers have been investigated. Zn(O,S) layers with three different [O]/([O] + [S]) ratios (0.4, 0.7, and 0.8)—and a combination of Zn(O,S) and CdS (“hybrid buffer layer”) were studied. In comparison to the CdS reference, the external quantum efficiency (EQE) of the Zn(O,S)-buffered devices increases in the short- and long-wavelength regions of the spectrum. However, the average EQE ranges below that of the CdS reference, and the devices show a low open-circuit voltage (VOC). By adding a very thin CdS layer (5 nm) between the absorber and the Zn(O,S) buffer, the VOC loss is completely avoided. Using thicker intermediate CdS layers result in a further device improvement, with VOC values above those of the CdS reference. X-ray photoelectron spectroscopy (XPS) measurements suggest that the thin CdS layer prevents damage to the absorber surface during the sputter deposition of the Zn(O,S) buffer. With the hybrid buffer configuration, a record VOC deficit, i.e., a minimum difference between bandgap energy Eg (divided by the elementary charge q) and VOC (Eg/q – VOC) of 519 mV could be obtained, i.e., the lowest value reported for kesterite solar cells to date. Thus, the hybrid buffer configuration is a promising approach to overcome one of the main bottlenecks of kesterite-based solar cells, while simultaneously also reducing the amount of cadmium needed in the device.
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