Modelling Insights of Sb<sub>2</sub>(S,Se)<sub>3</sub> Solar Cells Using Triazatruxene Hole Transport Layers

Abstract Sb 2 (S,Se) 3 is a promising thin‐film solar absorber with a tunable bandgap (1.3–1.7 eV) and earth‐abundant composition, yet its maximum reported efficiency (10.75%) in FTO/CdS/Sb 2 (S,Se) 3 /Spiro‐OMeTAD/Au remains below the Shockley‐Queisser limit. Moreover, the high cost of Spiro‐OMeTAD as an HTL limits commercialization. Herein cost‐effective triazatruxene‐based HTLs (CI‐B2, CI‐B3, TAT‐H, TAT‐TY1, TAT‐TY2) are introduced for the first time in Sb 2 (S,Se) 3 solar cells and optimize device performance using SCAPS‐1D. After replicating the experimental efficiency, optimization of HTL, ETL, and absorber parameters results in V OC (≈1 V), J SC &gt;30 mA cm −2 ), and FF (72–74%). Overall, efficiencies of 22.97%, 23.09%, 22.47%, 21.08%, 23.24%, and 23.11% are achieved for Spiro‐OMeTAD, CI‐B2, CI‐B3, TAT‐H, TAT‐TY1, and TAT‐TY2, respectively, owing to the reduced V OC loss (≈0.4 V), enhanced QE (&gt;70%), reduced recombination (by a factor of 3 × 10 18 cm −3 s −1 ), and stronger electric fields, positioning triazatruxene‐based HTLs as a cost‐effective alternative to Spiro‐OMeTAD, significantly boosting Sb 2 (S,Se) 3 solar cell performance.

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Publication Details

Journal
Advanced Theory and Simulations
Published
2025-06-09
DOI
https://doi.org/10.1002/adts.202500487
Citations
2
Primary Topic
Chalcogenide Semiconductor Thin Films
Type
article
Field-Weighted Citation Impact
1.46
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article

Modelling Insights of Sb2(S,Se)3 Solar Cells Using Triazatruxene Hole Transport Layers

H. Bencherif, Latha Marasamy, Aruna‐Devi Rasu Chettiar, Ponnusamy Sasikumar et al.
2 citations
Advanced Theory and Simulations
Chalcogenide Semiconductor Thin Films
1.46
article

Modelling Insights of Sb2(S,Se)3 Solar Cells Using Triazatruxene Hole Transport Layers

H. Bencherif, Latha Marasamy, Aruna‐Devi Rasu Chettiar, Ponnusamy Sasikumar, V George
article en
2 citations

Abstract

Abstract Sb 2 (S,Se) 3 is a promising thin‐film solar absorber with a tunable bandgap (1.3–1.7 eV) and earth‐abundant composition, yet its maximum reported efficiency (10.75%) in FTO/CdS/Sb 2 (S,Se) 3 /Spiro‐OMeTAD/Au remains below the Shockley‐Queisser limit. Moreover, the high cost of Spiro‐OMeTAD as an HTL limits commercialization. Herein cost‐effective triazatruxene‐based HTLs (CI‐B2, CI‐B3, TAT‐H, TAT‐TY1, TAT‐TY2) are introduced for the first time in Sb 2 (S,Se) 3 solar cells and optimize device performance using SCAPS‐1D. After replicating the experimental efficiency, optimization of HTL, ETL, and absorber parameters results in V OC (≈1 V), J SC &gt;30 mA cm −2 ), and FF (72–74%). Overall, efficiencies of 22.97%, 23.09%, 22.47%, 21.08%, 23.24%, and 23.11% are achieved for Spiro‐OMeTAD, CI‐B2, CI‐B3, TAT‐H, TAT‐TY1, and TAT‐TY2, respectively, owing to the reduced V OC loss (≈0.4 V), enhanced QE (&gt;70%), reduced recombination (by a factor of 3 × 10 18 cm −3 s −1 ), and stronger electric fields, positioning triazatruxene‐based HTLs as a cost‐effective alternative to Spiro‐OMeTAD, significantly boosting Sb 2 (S,Se) 3 solar cell performance.

Advanced Theory and SimulationsVol. 8(10)
Autonomous University of Queretaro (MX), University of Batna 1 (DZ), University of Tarapacá (CL), Saveetha University (IN)
Openalex Percentile: Top 17%
Chalcogenide Semiconductor Thin Films
1.46
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