Lead-Free Sr <sub>3</sub> MCl <sub>3</sub> (M = Sb, P) Perovskite Solar Cells: from First-Principles Calculations to Recombination-Aware Device Simulations

High Resolution Image Download MS PowerPoint Slide In this study, first-principles calculations were performed to explore structural, mechanical, electronic, carrier transport, and optical properties of strontium-based perovskites (Sr 3 MCl 3 (M = Sb, P)) using density functional theory (DFT). These calculations reveal that both materials are thermodynamically and mechanically stable. Employing the GGA-PBE functional, they possess a direct-band-gap semiconductor behavior with an energy of 1.704 eV (Sr 3 SbCl 3 ) and 1.677 eV (Sr 3 PCl 3 ). The analysis of the density of states (DOS) further corroborates the semiconducting behavior. Carrier mobility calculations indicate that electron/hole mobilities of 89.15/110.52 cm 2 /V·s are achieved for Sr 3 SbCl 3 and 137.16/100.60 cm 2 /V·s for Sr 3 PCl 3 . In the visible region, a light absorption coefficient above 10 5 cm –1 is reached for both materials, highlighting their suitability as an absorber layer (AL) in perovskite solar cells (PSCs). Considering band-to-band recombination (radiative and Auger), SCAPS-1D was used to conduct an inquiry into the photovoltaic performance of various devices, integrating different electron and hole transport layers (ETL/HTL): Ag/FTO/ETL/ uniform -AL/HTL/Ni. Among all configurations examined in this study, the Ag/FTO/IGZO/uniform-AL/Cu 2 O/Ni architecture achieves the highest photovoltaic performance parameters, upon optimization of AL thickness, AL-doping concentration, AL-bulk and interface defect densities, radiative recombination coefficient, and series/shunt resistances. The Sr 3 SbCl 3 -based PSC (Device I) attains a power conversion efficiency (PCE) of ∼25.80%, with an open-circuit voltage ( V OC ) of 1.31 V, a short-circuit current density ( J SC ) of 21.82 mA/cm 2, and a fill factor (FF) of 90.27%, whereas the Sr 3 PCl 3 -based PSC (Device II) achieves a PCE of approximatively 26.22%, with V OC = 1.28 V, J SC = 22.71 mA/cm 2, and FF = 90.09%. Finally, replacing the single uniform -AL with a graded -Sr 3 Sb 1– x P x Cl 3 AL (Device III), adopting linear and parabolic graded physical parameters, does not demonstrate marked improvements in device performance. Consequently, this study positions Sr 3 MCl 3 (M = Sb, P) perovskites as alternatives to lead-based ALs, which can constitute a suitable pathway for real-time experimentation of PSC.

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Journal
ACS Omega
Published
2026-06-17
DOI
https://doi.org/10.1021/acsomega.6c02217
Primary Topic
Perovskite Materials and Applications
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article
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article

Lead-Free Sr 3 MCl 3 (M = Sb, P) Perovskite Solar Cells: from First-Principles Calculations to Recombination-Aware Device Simulations

C. Saidi, M. Debbichi, N. Chaaben
ACS Omega
Perovskite Materials and Applications
article

Lead-Free Sr 3 MCl 3 (M = Sb, P) Perovskite Solar Cells: from First-Principles Calculations to Recombination-Aware Device Simulations

C. Saidi, M. Debbichi, N. Chaaben
article en

Abstract

High Resolution Image Download MS PowerPoint Slide In this study, first-principles calculations were performed to explore structural, mechanical, electronic, carrier transport, and optical properties of strontium-based perovskites (Sr 3 MCl 3 (M = Sb, P)) using density functional theory (DFT). These calculations reveal that both materials are thermodynamically and mechanically stable. Employing the GGA-PBE functional, they possess a direct-band-gap semiconductor behavior with an energy of 1.704 eV (Sr 3 SbCl 3 ) and 1.677 eV (Sr 3 PCl 3 ). The analysis of the density of states (DOS) further corroborates the semiconducting behavior. Carrier mobility calculations indicate that electron/hole mobilities of 89.15/110.52 cm 2 /V·s are achieved for Sr 3 SbCl 3 and 137.16/100.60 cm 2 /V·s for Sr 3 PCl 3 . In the visible region, a light absorption coefficient above 10 5 cm –1 is reached for both materials, highlighting their suitability as an absorber layer (AL) in perovskite solar cells (PSCs). Considering band-to-band recombination (radiative and Auger), SCAPS-1D was used to conduct an inquiry into the photovoltaic performance of various devices, integrating different electron and hole transport layers (ETL/HTL): Ag/FTO/ETL/ uniform -AL/HTL/Ni. Among all configurations examined in this study, the Ag/FTO/IGZO/uniform-AL/Cu 2 O/Ni architecture achieves the highest photovoltaic performance parameters, upon optimization of AL thickness, AL-doping concentration, AL-bulk and interface defect densities, radiative recombination coefficient, and series/shunt resistances. The Sr 3 SbCl 3 -based PSC (Device I) attains a power conversion efficiency (PCE) of ∼25.80%, with an open-circuit voltage ( V OC ) of 1.31 V, a short-circuit current density ( J SC ) of 21.82 mA/cm 2, and a fill factor (FF) of 90.27%, whereas the Sr 3 PCl 3 -based PSC (Device II) achieves a PCE of approximatively 26.22%, with V OC = 1.28 V, J SC = 22.71 mA/cm 2, and FF = 90.09%. Finally, replacing the single uniform -AL with a graded -Sr 3 Sb 1– x P x Cl 3 AL (Device III), adopting linear and parabolic graded physical parameters, does not demonstrate marked improvements in device performance. Consequently, this study positions Sr 3 MCl 3 (M = Sb, P) perovskites as alternatives to lead-based ALs, which can constitute a suitable pathway for real-time experimentation of PSC.

ACS Omega
University of Monastir (TN), Laboratoire de Physique Théorique de la Matière Condensée (FR), Laboratoire Lorrain de Chimie Moléculaire (FR), University of Kairouan (TN), Université de Lorraine (FR)
Openalex Percentile: Top 11%
Perovskite Materials and Applications
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