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Due to extended thermal carrier lifespan, small bandgap, and biocompatibility, tin (Sn)-based perovskite solar cells (PSCs) have garnered attention. Sn-based PSCs (nip-type), however, have performed poorly, mostly because of the careless application of metal oxide electron transport layers (ETLs), which were first created for lead-based PSCs of the nip type. The metal oxides deeper energy levels and oxygen vacancies are too responsible for this underperformance. In order to overcome these problems, we demonstrate a metal chalcogenide ETL, namely Sn(SSe), which prevents the oxidation of Sn and avoids the desorption of oxygen molecules. The variation of several charge transport layers is thoroughly analyzed in this work, indicating that SnS, TiO, and metal-doped Sn(SSe) are viable options to improve the efficiency of the FASnI (Energy gap (E) ≈ 1.41electron volt (eV) PSC. With Sn(SSe) as ETL and PTAA as Hole transport layer (HTL), the PSC's performance is maximized and the optimal performance device structure is attained. For our investigation, the optimal device structure is (Au/PTAA/FASnI/Sn(SSe)/FTO). We obtain an outstanding optimized value of Power conversion efficiency (PCE) 32.22%, Open circuit voltage (V) 1.2762 V, Fill factor (FF) 81.87%, and Short-circuit current density (J) 30.836 mA.cm by carefully evaluating and optimizing a number of variables, such as thickness of active layer, ETL and HTL, Acceptor density (N), Defect density (N) vs. thickness variation, Interface defect (IDD) and temperature variation. These findings provide a viable pathway for enhancing the efficiency of Sn-based PSCs.
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http://dx.doi.org/10.1038/s41598-025-93786-9 | DOI Listing |
J Phys Chem Lett
September 2025
Department of Chemistry and Chemical Biology, University of New Mexico, Albuquerque, New Mexico 87106, United States.
Defects significantly influence charge transport in CHNHPbI (MAPbI) perovskite solar cells, particularly at interfaces. Using quantum dynamics simulation, we reveal a distinct interstitial iodine (I) defect behavior at different positions in the TiO/MAPbI system. In the perovskite bulk-like region, I exhibits high mobility and dissociates detrimental iodine trimers, facilitating small-to-large polaron transition and promoting shallow trap formation.
View Article and Find Full Text PDFRSC Adv
September 2025
School of Engineering and Technology, National Textile University 37640 Faisalabad Pakistan
[This retracts the article DOI: 10.1039/D4RA01544D.].
View Article and Find Full Text PDFNanomicro Lett
September 2025
College of New Materials and New Energies, Shenzhen Technology University, Lantian Road 3002, Pingshan, 518118, Shenzhen, People's Republic of China.
The introduction of two-dimensional (2D) perovskite layers on top of three-dimensional (3D) perovskite films enhances the performance and stability of perovskite solar cells (PSCs). However, the electronic effect of the spacer cation and the quality of the 2D capping layer are critical factors in achieving the required results. In this study, we compared two fluorinated salts: 4-(trifluoromethyl) benzamidine hydrochloride (4TF-BA·HCl) and 4-fluorobenzamidine hydrochloride (4F-BA·HCl) to engineer the 3D/2D perovskite films.
View Article and Find Full Text PDFJ Chem Phys
September 2025
Quantum Chemistry Division, Yokohama City University, Seto 22-2, Kanazawa-Ku, Yokohama 236-0027, Kanagawa, Japan.
Perovskite-silicon tandem solar cells have attracted considerable attention owing to their high power conversion efficiency (PCE), which exceeds the limits of single-junction devices. This study focused on lead-free tin-based perovskites with iodine-bromine mixed anions. Bromide perovskites have a wide bandgap; therefore, they are promising light absorbers for perovskite-silicon tandem solar cells.
View Article and Find Full Text PDFAdv Mater
September 2025
School of Chemical Engineering and Light Industry, Guangdong University of Technology, Guangzhou, 510006, China.
Perovskite materials have revolutionized optoelectronics by virtue of their tunable bandgaps, exceptional optoelectronic properties, and structural flexibility. Notably, the state-of-the-art performance of perovskite solar cells has reached 27%, making perovskite materials a promising candidate for next-generation photovoltaic technology. Although numerous reviews regarding perovskite materials have been published, the existing reviews generally focus on individual material systems (e.
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