• Journal of Semiconductors
  • Vol. 41, Issue 6, 062701 (2020)
Peng Wang1、2, Gaofei Li3, Miao Wang3, Hong Li3, Jing Zheng3, Liyou Yang3, Yigang Chen1, Dongdong Li2, and Linfeng Lu2
Author Affiliations
  • 1School of Materials Science and Engineering, Shanghai University, Shanghai 200444, China
  • 2CAS Key Lab of Low-Carbon Conversion Science and Engineering, Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai 201210, China
  • 3Jinneng Clean Energy Limited Company, Lvliang 032100, China
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    DOI: 10.1088/1674-4926/41/6/062701 Cite this Article
    Peng Wang, Gaofei Li, Miao Wang, Hong Li, Jing Zheng, Liyou Yang, Yigang Chen, Dongdong Li, Linfeng Lu. Numerical study of mono-crystalline silicon solar cells with passivated emitter and rear contact configuration for the efficiency beyond 24% based on mass production technology[J]. Journal of Semiconductors, 2020, 41(6): 062701 Copy Citation Text show less

    Abstract

    Mono-crystalline silicon solar cells with a passivated emitter rear contact (PERC) configuration have attracted extensive attention from both industry and scientific communities. A record efficiency of 24.06% on p-type silicon wafer and mass production efficiency around 22% have been demonstrated, mainly due to its superior rear side passivation. In this work, the PERC solar cells with a p-type silicon wafer were numerically studied in terms of the surface passivation, quality of silicon wafer and metal electrodes. A rational way to achieve a 24% mass-production efficiency was proposed. Free energy loss analyses were adopted to address the loss sources with respect to the limit efficiency of 29%, which provides a guideline for the design and manufacture of a high-efficiency PERC solar cell.
    $ {J_{{\rm{rec}}}} = {J_{{\rm{0E}}}}{\left(\frac{np}{n_{\rm{i,eff}}^{\rm{2}}- 1}\right)}, $ (1)

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    $ {V_{\rm{OC}}} = \frac{{KT}}{q}{\rm{ln}}\left( {{\rm{1 + }}\frac{{{J_{{\rm{ph}}}}}}{{{J_{{\rm{rec}}}}}}} \right), $ (2)

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    $ {J_{{\rm{SC}}}} = {J_{{\rm{rec}}}}\left[ {{\rm{exp}}\left( {\frac{{qv}}{{nKT}}} \right) - 1} \right] - {J_{{\rm{ph}}}}, $ (3)

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    $ R = {R_{{\rm{Auger}}}}{\rm{ + }}{B_{{\rm{rad}}}}pn{\rm{ + }}{R_{{\rm{SRH}}}}{\rm{ + }}{\tau _{{\rm{b,fixed}}}}{\rm{(}}n-{n_{\rm{0}}}{\rm{),}} $ (4)

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    $ {R_{{\rm{SRH}}}}{\rm{ = }}\frac{{np-n_{{\rm{i,eff}}}^{\rm{2}}}}{{{\tau _{{\rm{p0}}}}\left( {{n_{\rm{1}}}{\rm{ + }}n} \right){\rm{ + }}{\tau _{{\rm{n0}}}}\left( {{p_{\rm{1}}}{\rm{ + }}p} \right)}}, $ (5)

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    Peng Wang, Gaofei Li, Miao Wang, Hong Li, Jing Zheng, Liyou Yang, Yigang Chen, Dongdong Li, Linfeng Lu. Numerical study of mono-crystalline silicon solar cells with passivated emitter and rear contact configuration for the efficiency beyond 24% based on mass production technology[J]. Journal of Semiconductors, 2020, 41(6): 062701
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