Mesoporous BaSnO3 layer based perovskite solar cells

2016 ◽  
Vol 52 (5) ◽  
pp. 970-973 ◽  
Author(s):  
Liangzheng Zhu ◽  
Zhipeng Shao ◽  
Jiajiu Ye ◽  
Xuhui Zhang ◽  
Xu Pan ◽  
...  
Keyword(s):  
Solar Cells ◽  
Electron Mobility ◽  
Perovskite Structure ◽  
Perovskite Solar Cells ◽  
Perovskite Oxide ◽  
High Electron ◽  
High Electron Mobility ◽  
Electron Transporting Layer

Perovskite oxide BaSnO3 with high electron mobility and a perovskite structure was first used as an electron-transporting layer in perovskite solar cells. After optimization, the resulting mp-BSO device can perform as well as the mp-TiO2 one and even better.

scholarly journals Fabrication of SnO2 by RF magnetron sputtering for electron transport layer of planar perovskite solar cells

2021 ◽  
Vol 2145 (1) ◽  
pp. 012027
Author(s):  
R Thanimkan ◽  
B Namnuan ◽  
S Chatraphorn
Keyword(s):  
Solar Cells ◽  
Electron Transport ◽  
Magnetron Sputtering ◽  
Electron Mobility ◽  
Perovskite Solar Cells ◽  
Rf Magnetron Sputtering ◽  
Transport Layer ◽  
Electron Transport Layer ◽  
High Electron ◽  
High Electron Mobility

Abstract The requirements of electron transport layer (ETL) for high efficiency Perovskite solar cells (PSCs) are, for example, appropriate band energy alignment, high electron mobility, high optical transmittance, high stability, and easy processing. SnO2 has attracted more attention as ETL for PSCs because it has diverse advantages, e.g., wide bandgap energy, excellent optical and chemical stability, high transparency, high electron mobility, and easy preparation. The SnO2 ETL was fabricated by RF magnetron sputtering technique to ensure the chemical composition and uniform layer thickness when compared to the use of chemical solution via spin-coating method. The RF power was varied from 60 - 150 W. The Ar sputtering gas pressure was varied from 1 × 10−3 - 6 × 10−3 mbar while keeping O2 partial pressure at 1 × 10−4 mbar. The thickness of SnO2 layer decreases as the Ar gas pressure increases resulting in the increase of sheet resistance. The surface morphology and optical transmission of the SnO2 ETL were investigated. It was found that the optimum thickness of SnO2 layer was approximately 35 - 40 nm. The best device shows Jsc = 27.4 mA/cm2, Voc = 1.03 V, fill factor = 0.63, and efficiency = 17.7%.

High electron mobility ZnO film for high-performance inverted polymer solar cells

2015 ◽  
Vol 106 (16) ◽  
pp. 163902 ◽  
Author(s):  
Peiwen Lv ◽  
Shan-Ci Chen ◽  
Qingdong Zheng ◽  
Feng Huang ◽  
Kai Ding
Keyword(s):  
Solar Cells ◽  
Electron Mobility ◽  
High Performance ◽  
Polymer Solar Cells ◽  
High Electron ◽  
Zno Film ◽  
High Electron Mobility ◽  
Inverted Polymer Solar Cells

A–D–A small molecule acceptors with ladder-type arenes for organic solar cells

2018 ◽  
Vol 6 (19) ◽  
pp. 8839-8854 ◽  
Author(s):  
Dan He ◽  
Fuwen Zhao ◽  
Li Jiang ◽  
Chunru Wang
Keyword(s):  
Solar Cells ◽  
Power Conversion Efficiency ◽  
Small Molecule ◽  
High Power ◽  
Organic Solar Cells ◽  
Electron Mobility ◽  
Power Conversion ◽  
High Electron ◽  
High Power Conversion Efficiency ◽  
High Electron Mobility

A–D–A small molecule acceptors possess strong absorption in the visible or NIR region, low bandgaps, relatively high electron mobility and proper miscibility with donors, which enables the achievement of high power conversion efficiency for organic solar cells based on these molecules.

An efficient and thickness insensitive cathode interface material for high performance inverted perovskite solar cells with 17.27% efficiency

2017 ◽  
Vol 5 (24) ◽  
pp. 5949-5955 ◽  
Author(s):  
Sen Peng ◽  
Jingsheng Miao ◽  
Imran Murtaza ◽  
Liang Zhao ◽  
Zhao Hu ◽  
...  
Keyword(s):  
Energy Level ◽  
Electron Mobility ◽  
High Performance ◽  
Power Conversion ◽  
Control Cell ◽  
Perovskite Solar Cells ◽  
High Electron ◽  
Lumo Energy ◽  
High Electron Mobility ◽  
Water Alcohol

A thickness insensitive water/alcohol soluble small molecular, PN6, exhibits high electron mobility with deep LUMO energy level, and effectively decrease the work function of the cathode. Those properties significantly enhance the power conversion efficiency from 8.73% (control cell) to 17.27%.

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