Theoretical Optimization of Lateral Heterojunction Perovskite Solar Cells: A Structural Perspective

Lateral heterojunction perovskite solar cells are well-known for their high stability. However, their efficiency is very low compared to traditional solar cells. Hence, it is crucial to theoretically study lateral heterojunction perovskite solar cells to find the reason for low efficiency and improve their performance. Therefore, in this study we simulated the lateral heterojunction perovskite solar cells to find optimal sizes and doping concentrations. We used TiO<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> as Electron Transport Layer (ETL) and NiO<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> as Hole Transport Layer (HTL) to extract charges from CH<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub>NH<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub>PbI<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> perovskite layer. We varied the thickness, width and doping concentration of each layer. According to the obtained results, optimal thicknesses are 40 nm for ETL and HTL, and 900 nm for perovskite layer. In lateral heterojunctions, the width of each layer is one of the key parameters that can significantly influence photoelectric parameters of the solar cell. We have found that the optimal width of ETL and HTL is 1200 nm. Optimal donor and acceptor concentrations are equal to 1×10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">15</sup> cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-3</sup> in the n-region and 1×10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">16</sup> cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-3</sup> in the p-region. A lateral heterojunction solar cell with optimal size and doping concentrations achieved 29.9% efficiency, an open circuit voltage of 1.172 V, a short circuit current of 18.33 mA/cm² and a fill factor of 88.06%.

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Journal
IEEE Access
Published
2025-01-01
DOI
https://doi.org/10.1109/access.2025.3571476
Primary Topic
Perovskite Materials and Applications
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article
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article

Theoretical Optimization of Lateral Heterojunction Perovskite Solar Cells: A Structural Perspective

Irodakhon Gulomova, Oussama Accouche, Rayimjon Aliev
3 links
IEEE Access
Perovskite Materials and Applications
article

Theoretical Optimization of Lateral Heterojunction Perovskite Solar Cells: A Structural Perspective

Irodakhon Gulomova, Oussama Accouche, Rayimjon Aliev
article en

Abstract

Lateral heterojunction perovskite solar cells are well-known for their high stability. However, their efficiency is very low compared to traditional solar cells. Hence, it is crucial to theoretically study lateral heterojunction perovskite solar cells to find the reason for low efficiency and improve their performance. Therefore, in this study we simulated the lateral heterojunction perovskite solar cells to find optimal sizes and doping concentrations. We used TiO<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> as Electron Transport Layer (ETL) and NiO<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> as Hole Transport Layer (HTL) to extract charges from CH<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub>NH<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub>PbI<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> perovskite layer. We varied the thickness, width and doping concentration of each layer. According to the obtained results, optimal thicknesses are 40 nm for ETL and HTL, and 900 nm for perovskite layer. In lateral heterojunctions, the width of each layer is one of the key parameters that can significantly influence photoelectric parameters of the solar cell. We have found that the optimal width of ETL and HTL is 1200 nm. Optimal donor and acceptor concentrations are equal to 1×10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">15</sup> cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-3</sup> in the n-region and 1×10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">16</sup> cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-3</sup> in the p-region. A lateral heterojunction solar cell with optimal size and doping concentrations achieved 29.9% efficiency, an open circuit voltage of 1.172 V, a short circuit current of 18.33 mA/cm² and a fill factor of 88.06%.

IEEE AccessVol. 13
Andijan State University (UZ), American University of the Middle East (KW)
Affordable and clean energy
Openalex Percentile: Top 91%
Perovskite Materials and Applications
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