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Theoretical Analysis of the Effect of the Interfacial MoSe<sub>2</sub>Layer in CIGS-Based Solar Cells
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作者 Adama Sylla N’Guessan Armel Ignace +1 位作者 Touré Siaka Jean-Pierre Vilcot 《Open Journal of Modelling and Simulation》 2021年第4期339-350,共12页
<span style="font-family:Verdana;">The aim of this work is to analyze the influence of the interfacial MoSe</span><sub><span style="font-family:Verdana;">2</span></... <span style="font-family:Verdana;">The aim of this work is to analyze the influence of the interfacial MoSe</span><sub><span style="font-family:Verdana;">2</span></sub><span style="font-family:Verdana;"> layer </span><span style="font-family:Verdana;">on </span><span style="font-family:Verdana;"><span>the performance of a /n-ZnO/i-ZnO/n-Zn(O,S)/p-CIGS/p</span><sup><span>+</span></sup><span>-MoSe</span><sub><span>2</span></sub><span>/Mo/SLG</span></span><span style="font-family:Verdana;"> solar cell. In this investigation, the numerical simulation software AFORS-</span><span style="font-family:Verdana;">HET is used to calculate the electrical characteristics of the cell with and</span><span style="font-family:Verdana;"> without this MoSe</span><span style="font-family:Verdana;"><sub>2</sub></span><span style="font-family:Verdana;"> layer. Different reported experimental works have highlighted the presence of a thin-film MoSe</span><span style="font-family:Verdana;"><sub>2</sub></span><span style="font-family:Verdana;"> layer at the CIGS/Mo contact interface. Under a tunneling effect, this MoSe</span><span style="font-family:Verdana;"><sub>2</sub></span><span style="font-family:Verdana;"> layer transforms the Schottky CIGS/Mo contact nature into a quasi-ohmic one. Owing to a heavily p-doping, the MoSe</span><span style="font-family:Verdana;"><sub>2</sub></span><span style="font-family:Verdana;"> thin layer allows better transport of majority carrier, tunneling them from CIGS to Mo. Moreover, the bandgap of MoSe</span><span style="font-family:Verdana;"><sub>2</sub></span><span style="font-family:Verdana;"> is wider than that of the CIGS absorbing layer, such that an electric field is generated close to the back surface. The presence of this electric field reduces carrier recombination at the interface. Under these conditions, we examined the performance of the cell with and without MoSe</span><span style="font-family:Verdana;"><sub>2</sub></span><span style="font-family:Verdana;"> layer. When the thickness of the CIGS absorber is in the range from 3.5 μm down to 1.5 μm, the efficiency of the cell with a MoSe</span><span style="font-family:Verdana;"><sub>2</sub></span><span style="font-family:Verdana;"> interfacial layer remains almost constant, about 24.6%, while that of the MoSe</span><sub><span style="font-family:Verdana;">2</span></sub><span style="font-family:Verdana;">-free solar cell decreases from 24.6% to 23.4%. Besides, a Schottky barrier height larger than 0.45 eV severely affects the fill factor and open circuit voltage of the solar cell with MoSe</span><sub><span style="font-family:Verdana;">2</span></sub><span style="font-family:Verdana;"> interface layer compared to the MoSe</span><span style="font-family:Verdana;"><sub>2</sub></span><span style="font-family:Verdana;">-free solar cell.</span> 展开更多
关键词 CIGS Numerical Simulation AFORS-HET Quasi-Ohmic Contact Schottky Contact MoSe2 Tunnel Layer
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