Mahasen H. Albelbeisi, Saleh Chebaane, Sana Ben Khalifa, Norah A. M. Alsaif
The primary causes of the high cost of perovskite solar cells are metal electrodes and hole transport layers. In this theoretical work, we examine the outputs of a hole transport layer‐free carbon‐based solar cell with an FTO/ETL/Cs 2 PtI 6 /Carbon electrode structure using the Solar Cell Capacitance Simulator (SCAPS‐1D). The paper studied various carbon electrode types‐Graphene/Carbon Black (G/CB) (5 eV), Graphene (4.9 eV), Graphene Oxide (GO) (4.8 eV), and Bio‐carbon (4.5 eV)‐ and electron transport layers‐SnO 2 , TiO 2 , LBSO, and WO 3 . The studied parameters included perovskite and ETL layer thickness, doping density, and defect density. The outputs showed that the best PCE of 15.50% resulted from using G/CB electrode and TiO 2 as the ETL, with a thickness of 0.09 µm, and a doping density of 10 × 10 19 cm −3 . Additionally, for the Cs 2 PtI 6 absorber layer, a Cs 2 PtI 6 composition with a thickness of 1.2 µm, a defect density of 1× 10 15 cm −3 , and a doping density of 10 × 10 12 cm −3 demonstrated superior performance, resulting in a PCE of 15.50%. These findings suggest that the FTO/TiO 2 /Cs 2 PtI 6 /G/CB structure, particularly with optimized TiO 2 and Cs 2 PtI 6 layers, holds great potential for hole transport layer‐free‐carbon‐based solar cell fabrication. Furthermore, machine learning models with a random forest algorithm evaluated the relative importance of the features on cell efficiency, and predicted the efficiency of the suggested configuration with R 2 of 0.93 underscoring the potential of machine learning in enhancing solar cell design and performance.
{"title":"Advancing HTL‐Free Cs 2 PtI 6 Carbon Perovskite Solar Cells: Insights from Hybrid Simulation and Machine Learning","authors":"Mahasen H. Albelbeisi, Saleh Chebaane, Sana Ben Khalifa, Norah A. M. Alsaif","doi":"10.1002/adts.202501860","DOIUrl":"https://doi.org/10.1002/adts.202501860","url":null,"abstract":"The primary causes of the high cost of perovskite solar cells are metal electrodes and hole transport layers. In this theoretical work, we examine the outputs of a hole transport layer‐free carbon‐based solar cell with an FTO/ETL/Cs <jats:sub>2</jats:sub> PtI <jats:sub>6</jats:sub> /Carbon electrode structure using the Solar Cell Capacitance Simulator (SCAPS‐1D). The paper studied various carbon electrode types‐Graphene/Carbon Black (G/CB) (5 eV), Graphene (4.9 eV), Graphene Oxide (GO) (4.8 eV), and Bio‐carbon (4.5 eV)‐ and electron transport layers‐SnO <jats:sub>2</jats:sub> , TiO <jats:sub>2</jats:sub> , LBSO, and WO <jats:sub>3</jats:sub> . The studied parameters included perovskite and ETL layer thickness, doping density, and defect density. The outputs showed that the best PCE of 15.50% resulted from using G/CB electrode and TiO <jats:sub>2</jats:sub> as the ETL, with a thickness of 0.09 µm, and a doping density of 10 × 10 <jats:sup>19</jats:sup> cm <jats:sup>−3</jats:sup> . Additionally, for the Cs <jats:sub>2</jats:sub> PtI <jats:sub>6</jats:sub> absorber layer, a Cs <jats:sub>2</jats:sub> PtI <jats:sub>6</jats:sub> composition with a thickness of 1.2 µm, a defect density of 1× 10 <jats:sup>15</jats:sup> cm <jats:sup>−3</jats:sup> , and a doping density of 10 × 10 <jats:sup>12</jats:sup> cm <jats:sup>−3</jats:sup> demonstrated superior performance, resulting in a PCE of 15.50%. These findings suggest that the FTO/TiO <jats:sub>2</jats:sub> /Cs <jats:sub>2</jats:sub> PtI <jats:sub>6</jats:sub> /G/CB structure, particularly with optimized TiO <jats:sub>2</jats:sub> and Cs <jats:sub>2</jats:sub> PtI <jats:sub>6</jats:sub> layers, holds great potential for hole transport layer‐free‐carbon‐based solar cell fabrication. Furthermore, machine learning models with a random forest algorithm evaluated the relative importance of the features on cell efficiency, and predicted the efficiency of the suggested configuration with R <jats:sup>2</jats:sup> of 0.93 underscoring the potential of machine learning in enhancing solar cell design and performance.","PeriodicalId":7219,"journal":{"name":"Advanced Theory and Simulations","volume":"9 1","pages":""},"PeriodicalIF":3.3,"publicationDate":"2025-12-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145731397","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The critical behavior of (1−x) LSMO/xNaF composites with x = 0, 0.05, 0.15, and 0.20 near the second‐order paramagnetic–ferromagnetic transition is investigated through a combination of Arrott–Noakes formalism (ANF) and Kouvel–Fisher (KF) analysis. Critical exponents ( β , γ ) are determined iteratively to be (1.0004, 0.3406), (1.1593, 0.6230), (1.0467, 0.4391), and (1.0479, 0.4673) for (1‐x)LSMO/xNaF with x = 0, 0.05, 0.15, and 0.20, respectively. Furthermore, magnetocaloric entropy changes , computed via Landau theory, exhibited strong correspondence with Maxwell relation results, with minor discrepancies at high fields attributed to saturation effects. Overall, the results highlight the robustness of Landau phenomenology in describing criticality and magnetocaloric behavior, while revealing subtle doping‐induced modifications in exchange interactions.
{"title":"Critical Behavior and Magnetocaloric Simulation in LSMO/NaF Composites Using Landau Theory","authors":"Mohamed Hsini, Nadia Zaidi, Amel Haouas","doi":"10.1002/adts.202501677","DOIUrl":"https://doi.org/10.1002/adts.202501677","url":null,"abstract":"The critical behavior of (1−x) LSMO/xNaF composites with x = 0, 0.05, 0.15, and 0.20 near the second‐order paramagnetic–ferromagnetic transition is investigated through a combination of Arrott–Noakes formalism (ANF) and Kouvel–Fisher (KF) analysis. Critical exponents ( <jats:italic>β</jats:italic> , <jats:italic>γ</jats:italic> ) are determined iteratively to be (1.0004, 0.3406), (1.1593, 0.6230), (1.0467, 0.4391), and (1.0479, 0.4673) for (1‐x)LSMO/xNaF with x = 0, 0.05, 0.15, and 0.20, respectively. Furthermore, magnetocaloric entropy changes , computed via Landau theory, exhibited strong correspondence with Maxwell relation results, with minor discrepancies at high fields attributed to saturation effects. Overall, the results highlight the robustness of Landau phenomenology in describing criticality and magnetocaloric behavior, while revealing subtle doping‐induced modifications in exchange interactions.","PeriodicalId":7219,"journal":{"name":"Advanced Theory and Simulations","volume":"6 1","pages":""},"PeriodicalIF":3.3,"publicationDate":"2025-12-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145711415","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A conceptual design of a two-terminal tandem solar cell featuring ZrS2 as the top absorber and CH3NH3SnI3 perovskite as the bottom absorber layer of the two sub-cells. Color-coded incident photon paths illustrate wavelength-selective absorption in each sub-cell, highlighting efficient spectral utilization and enhanced energy conversion performance. More details can be found in the Research Article by Avijit Kumar, Shyamal Chatterjee, and co-workers (DOI: 10.1002/adts.202501325).