硅太阳能电池体扩散长度和有效后表面复合速度的映射

R. Jain, S. Behera, K. Sreejith, A. Kottantharayil, P. Basu, A. Sharma
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引用次数: 7

摘要

利用期望波长下的光谱响应(SR),对AI-BSF和PERC Si太阳能电池的体区扩散长度(L)和有效后表面复合速度(SRV)进行了映射。采用光束感应电流(LBIC)技术生成细胞面积(6”x6”)上的SR和反射率(R)图。利用MATLAB工具将SR和R的空间图转换为L和SRV。我们发现(i) L在多晶细胞中的分布范围很广(150-600 $\mu$m),而在单晶细胞中的分布范围很窄(450-600$\mu$m);(ii) PERC电池(单晶120-250 cm/秒,多晶100-250 cm/秒)和AI-BSF电池(单晶320-400 cm/秒,多晶250-350 cm/秒)的SRV值由于背面钝化质量的不同而存在相当大的差异。用所提出的方法研究了三种电池效率分别为17.6%、17.9%和18.1%的多晶AI-BSF Si太阳能电池,并证明了效率缺陷主要是由于大块材料存在缺陷和背表面钝化不良。
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Mapping of Bulk Diffusion Length and Effective Back Surface Recombination Velocity in Silicon Solar Cells
Mapping of diffusion length (L) in the bulk region and effective back surface recombination velocity (SRV) in AI-BSF and PERC Si solar cells has been carried out by utilizing the spectral response (SR) at desired wavelengths. Light beam induced current (LBIC) technique was used to generate the maps of SR and reflectivity (R) on cell area (6” x6”). MATLAB tool was used to convert the spatial maps of SR and R into L and SRV. We found that (i) the distribution of L in multi-crystalline cells varied from grain to grain in wide range (150-600 $\mu$m) while in mono-crystalline cells, it varied in rather narrow range (450-600$\mu$m); (ii) the values of SRV for PERC cells (120-250 cm/sec for mono-crystalline and 100-250 cm/sec for multi-crystalline) and AI-BSF cells (320-400 cm/sec for mono-crystalline and 250-350 cm/sec for multi-crystalline) differ by considerable magnitude due to passivation quality at back side. Three multi-crystalline AI-BSF Si solar cells of cell efficiencies 17.6%, 17.9% and 18.1% were investigated with the proposed methodology and demonstrated that the efficiency deficit is primarily due to defects present in bulk material and poor back surface passivation.
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