AI-assisted optimization of lead-free Rb <sub>2</sub> SiX <sub>6</sub> (X = F, Cl, Br, and I) perovskite solar cells with a 2D buffer layer design using DFT and SCAPS-1D

In this work, the potential of the environmentally benign double halide perovskite Rb<sub>2</sub>SiX<sub>6</sub> (X = F, Cl, Br, and I) as a solar cell absorber is investigated through the combined use of density functional theory (DFT), SCAPS-1D modeling, and machine learning techniques. Detailed DFT analysis indicates that Rb<sub>2</sub>SiBr<sub>6</sub> crystallizes in a stable cubic structure with a direct bandgap of ∼1.65 eV, making it the most suitable among Rb<sub>2</sub>SiF<sub>6</sub>, Rb<sub>2</sub>SiCl<sub>6</sub>, Rb<sub>2</sub>SiBr<sub>6</sub>, and Rb<sub>2</sub>SiI<sub>6</sub> for visible light absorption. SCAPS-1D modeling reveals that device performance depends strongly on absorber thickness, doping concentration, and interface defect density. In the absence of a back surface field (BSF) layer, the device achieved a <i>V</i><sub>OC</sub> of 1.13 V, a <i>J</i><sub>SC</sub> of 21.28 mA cm<sup>-2</sup>, an FF of 85.66%, and a PCE of 20.56% with a two-dimensional (2D) WS<sub>2</sub> buffer layer. Introducing a Spiro-OMeTAD BSF layer further boosts performance, increasing <i>V</i><sub>OC</sub> to 1.25 V and <i>J</i><sub>SC</sub> to 22.93 mA cm<sup>-2</sup> with a slight change in FF to 84.64%, resulting in a PCE of 24.27%. The BSF layer also enhances thermal stability, suppresses recombination losses, and improves carrier extraction under varied operating conditions. Machine learning, particularly Random Forest with SHAP analysis, highlights electron affinity and conduction band density of states as the most influential factors for device efficiency. While simulations predict efficiencies above 24%, experimental validation is essential to address fabrication and long-term stability challenges, supporting Rb<sub>2</sub>SiBr<sub>6</sub> as a non-toxic, scalable photovoltaic candidate.

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Publication Details

Journal
Dalton Transactions
Published
2026-01-01
DOI
https://doi.org/10.1039/d5dt02363g
Citations
1
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
21.93
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article

AI-assisted optimization of lead-free Rb 2 SiX 6 (X = F, Cl, Br, and I) perovskite solar cells with a 2D buffer layer design using DFT and SCAPS-1D

Shamshad Alam, Ahmad Irfan, Aijaz Rasool Chaudhry, Tanvir Al Galib et al.
1 citations
Dalton Transactions
Perovskite Materials and Applications
21.93
article

AI-assisted optimization of lead-free Rb 2 SiX 6 (X = F, Cl, Br, and I) perovskite solar cells with a 2D buffer layer design using DFT and SCAPS-1D

Shamshad Alam, Ahmad Irfan, Aijaz Rasool Chaudhry, Tanvir Al Galib, Md Masum Mia, Md. Ferdous Rahman, Rihan Akter, Abdullah M Alharbi
article en
1 citations

Abstract

In this work, the potential of the environmentally benign double halide perovskite Rb<sub>2</sub>SiX<sub>6</sub> (X = F, Cl, Br, and I) as a solar cell absorber is investigated through the combined use of density functional theory (DFT), SCAPS-1D modeling, and machine learning techniques. Detailed DFT analysis indicates that Rb<sub>2</sub>SiBr<sub>6</sub> crystallizes in a stable cubic structure with a direct bandgap of ∼1.65 eV, making it the most suitable among Rb<sub>2</sub>SiF<sub>6</sub>, Rb<sub>2</sub>SiCl<sub>6</sub>, Rb<sub>2</sub>SiBr<sub>6</sub>, and Rb<sub>2</sub>SiI<sub>6</sub> for visible light absorption. SCAPS-1D modeling reveals that device performance depends strongly on absorber thickness, doping concentration, and interface defect density. In the absence of a back surface field (BSF) layer, the device achieved a <i>V</i><sub>OC</sub> of 1.13 V, a <i>J</i><sub>SC</sub> of 21.28 mA cm<sup>-2</sup>, an FF of 85.66%, and a PCE of 20.56% with a two-dimensional (2D) WS<sub>2</sub> buffer layer. Introducing a Spiro-OMeTAD BSF layer further boosts performance, increasing <i>V</i><sub>OC</sub> to 1.25 V and <i>J</i><sub>SC</sub> to 22.93 mA cm<sup>-2</sup> with a slight change in FF to 84.64%, resulting in a PCE of 24.27%. The BSF layer also enhances thermal stability, suppresses recombination losses, and improves carrier extraction under varied operating conditions. Machine learning, particularly Random Forest with SHAP analysis, highlights electron affinity and conduction band density of states as the most influential factors for device efficiency. While simulations predict efficiencies above 24%, experimental validation is essential to address fabrication and long-term stability challenges, supporting Rb<sub>2</sub>SiBr<sub>6</sub> as a non-toxic, scalable photovoltaic candidate.

Dalton TransactionsVol. 55(7)
Begum Rokeya University (BD), Shaqra University (SA), University of Bisha (SA), King Khalid University (SA)
Openalex Percentile: Top 3%
Perovskite Materials and Applications
21.93
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