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Influence of Window Layers on the Spectral Evolution of the Total Current Flowing Through a Solar Cell Based on Lead-Free Perovskite Materials

Received: 14 May 2025     Accepted: 28 May 2025     Published: 23 June 2025
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Abstract

In this work a modeling study of photovoltaic devices based on lead-free CH3 NH3 Sn(1-y)Gey I3 perovskite materials, is carried out with different window layers. The transport window layers materials used are ZnO, TiO2 and SnO2. They enable minority charge carriers to be transported to the active perovskite layer and collected there. The study also focuses on the influence of geometric parameters such as the diffusion length of minority charge carriers, the surface recombination velocity and the thickness of the window layers on the performance of the devices. The photovoltaic devices have first been modeled using the ZnO window layer in the multijunction ZnO(n+)/Cu2O(n)/CH3NH3Sn(1-y)GeyI3(p) structure. The ZnO window layer was then successively substituted by the TiO2 and SnO2 layers, leading thus to TiO2 (n+)/Cu2 O(n)/CH3NH3Sn(1-y)GeyI3(p) and SnO2 (n+)/Cu2 O(n)/ CH3 NH3 Sn(1-y)Gey I3 (p) photovoltaic structures, respectively. The CH3 NH3 Sn(1-y)Gey I3 perovskite absorber layers considered in these structures contain a germanium content varying from 0 to 1. Our study showed that the best performances are obtained for a germanium content of around 0.25, corresponding to 65.8%, 49.7% and 64.5%, for ZnO, SnO2 and TiO2 window layers, respectively.

Published in International Journal of Materials Science and Applications (Volume 14, Issue 3)
DOI 10.11648/j.ijmsa.20251403.14
Page(s) 79-88
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2025. Published by Science Publishing Group

Keywords

Lead-Free Perovskite, Internal Quantum Efficiency, Solar Cell

References
[1] M. G. Ju, J. Dai, L. Ma, X. C. Zeng, Lead-free mixed tin and germanium perovskites for photovoltaic application, J. Am. Chem. Soc., 139 (2017) 8038−8043.
[2] P. Cheng, T. Wu, J. Liu, W. Q. Deng, K. Han, Lead-free, two-dimensional mixed germanium and tin perovskites, J. Phys. Chem. Lett., 9 (2018) 2518−2522.
[3] S. Nagane, D. Ghosh, R. L. Z. Hoye, B. Zhao, S. Ahmad, A. B. Walker, M. S. Islam, S. Ogale, A. Sadhanala, Lead-free perovskite semiconductors based on germanium-tin solid solutions: Structural and optoelectronic properties, J. Phys. Chem. C, 122 (2018) 5940−5947.
[4] L. Zhang, W. Liang, How the structures and properties of twodimensional layered perovskites MAPbI3 and CsPbI3 vary with the number of layers, J. Phys. Chem. Lett., 8 (2017) 1517-1523.
[5] M. Kar, R. Sarkar, S. Pal, P. Sarkar, Lead Free Two-Dimensional Mixed Tin and Germanium Halide Perovskites for Photovoltaic Applications, J. Phys. Chem., 125 (2021) 74−81.
[6] S. Seck, A. Sow, M. S. Mané, A. Ndiaye, E. M. Keita, B. Ndiaye, B. Mbow, and C. Sène, Modeling and Analysis of a Mixed Sn-Ge Lead Free Perovskite Based Solar Cells, American Journal of Energy Research, 12 (1) (2024) 1-7.
[7] Z. Shi, J. Guo, Y. Chen, Q. Li, Y. Pan, H. Zhang, Y. Xia, W. Huang, Lead-free organic-inorganic hybrid perovskites for photovoltaic applications: Recent advances and perspectives, Adv. Mater., 29 (2017) 1605005.
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    Seck, S., Sow, A., Mane, M. S., Faye, M., Keita, E. H. M., et al. (2025). Influence of Window Layers on the Spectral Evolution of the Total Current Flowing Through a Solar Cell Based on Lead-Free Perovskite Materials. International Journal of Materials Science and Applications, 14(3), 79-88. https://doi.org/10.11648/j.ijmsa.20251403.14

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    ACS Style

    Seck, S.; Sow, A.; Mane, M. S.; Faye, M.; Keita, E. H. M., et al. Influence of Window Layers on the Spectral Evolution of the Total Current Flowing Through a Solar Cell Based on Lead-Free Perovskite Materials. Int. J. Mater. Sci. Appl. 2025, 14(3), 79-88. doi: 10.11648/j.ijmsa.20251403.14

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    AMA Style

    Seck S, Sow A, Mane MS, Faye M, Keita EHM, et al. Influence of Window Layers on the Spectral Evolution of the Total Current Flowing Through a Solar Cell Based on Lead-Free Perovskite Materials. Int J Mater Sci Appl. 2025;14(3):79-88. doi: 10.11648/j.ijmsa.20251403.14

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  • @article{10.11648/j.ijmsa.20251403.14,
      author = {Saliou Seck and Alioune Sow and Mamadou Salif Mane and Modou Faye and El Hadji Mamadou Keita and Amadou Ndiaye and Bachirou Ndiaye and Babacar Mbow and Cheikh Sene},
      title = {Influence of Window Layers on the Spectral Evolution of the Total Current Flowing Through a Solar Cell Based on Lead-Free Perovskite Materials
    },
      journal = {International Journal of Materials Science and Applications},
      volume = {14},
      number = {3},
      pages = {79-88},
      doi = {10.11648/j.ijmsa.20251403.14},
      url = {https://doi.org/10.11648/j.ijmsa.20251403.14},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ijmsa.20251403.14},
      abstract = {In this work a modeling study of photovoltaic devices based on lead-free CH3 NH3 Sn(1-y)Gey I3 perovskite materials, is carried out with different window layers. The transport window layers materials used are ZnO, TiO2 and SnO2. They enable minority charge carriers to be transported to the active perovskite layer and collected there. The study also focuses on the influence of geometric parameters such as the diffusion length of minority charge carriers, the surface recombination velocity and the thickness of the window layers on the performance of the devices. The photovoltaic devices have first been modeled using the ZnO window layer in the multijunction ZnO(n+)/Cu2O(n)/CH3NH3Sn(1-y)GeyI3(p) structure. The ZnO window layer was then successively substituted by the TiO2 and SnO2 layers, leading thus to TiO2 (n+)/Cu2 O(n)/CH3NH3Sn(1-y)GeyI3(p) and SnO2 (n+)/Cu2 O(n)/ CH3 NH3 Sn(1-y)Gey I3 (p) photovoltaic structures, respectively. The CH3 NH3 Sn(1-y)Gey I3 perovskite absorber layers considered in these structures contain a germanium content varying from 0 to 1. Our study showed that the best performances are obtained for a germanium content of around 0.25, corresponding to 65.8%, 49.7% and 64.5%, for ZnO, SnO2 and TiO2 window layers, respectively.
    },
     year = {2025}
    }
    

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  • TY  - JOUR
    T1  - Influence of Window Layers on the Spectral Evolution of the Total Current Flowing Through a Solar Cell Based on Lead-Free Perovskite Materials
    
    AU  - Saliou Seck
    AU  - Alioune Sow
    AU  - Mamadou Salif Mane
    AU  - Modou Faye
    AU  - El Hadji Mamadou Keita
    AU  - Amadou Ndiaye
    AU  - Bachirou Ndiaye
    AU  - Babacar Mbow
    AU  - Cheikh Sene
    Y1  - 2025/06/23
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    DO  - 10.11648/j.ijmsa.20251403.14
    T2  - International Journal of Materials Science and Applications
    JF  - International Journal of Materials Science and Applications
    JO  - International Journal of Materials Science and Applications
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    EP  - 88
    PB  - Science Publishing Group
    SN  - 2327-2643
    UR  - https://doi.org/10.11648/j.ijmsa.20251403.14
    AB  - In this work a modeling study of photovoltaic devices based on lead-free CH3 NH3 Sn(1-y)Gey I3 perovskite materials, is carried out with different window layers. The transport window layers materials used are ZnO, TiO2 and SnO2. They enable minority charge carriers to be transported to the active perovskite layer and collected there. The study also focuses on the influence of geometric parameters such as the diffusion length of minority charge carriers, the surface recombination velocity and the thickness of the window layers on the performance of the devices. The photovoltaic devices have first been modeled using the ZnO window layer in the multijunction ZnO(n+)/Cu2O(n)/CH3NH3Sn(1-y)GeyI3(p) structure. The ZnO window layer was then successively substituted by the TiO2 and SnO2 layers, leading thus to TiO2 (n+)/Cu2 O(n)/CH3NH3Sn(1-y)GeyI3(p) and SnO2 (n+)/Cu2 O(n)/ CH3 NH3 Sn(1-y)Gey I3 (p) photovoltaic structures, respectively. The CH3 NH3 Sn(1-y)Gey I3 perovskite absorber layers considered in these structures contain a germanium content varying from 0 to 1. Our study showed that the best performances are obtained for a germanium content of around 0.25, corresponding to 65.8%, 49.7% and 64.5%, for ZnO, SnO2 and TiO2 window layers, respectively.
    
    VL  - 14
    IS  - 3
    ER  - 

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Author Information
  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

  • Department of Physics, Faculty of Sciences and Technology, Semiconductors and Solar Energy Laboratory, Cheikh Anta Diop University, Dakar, Senegal

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