First-principles study of La and Mg doped/co-doped TiO2 for tailoring trap states in the electron transport layer of perovskite solar cells

Doping TiO 2 with La and Mg shows promise in enhancing its performance as an electron transport layer (ETL) in perovskite solar cells. Yet, a comprehensive understanding of the specific contributions of these dopants to TiO 2 properties remains elusive. In the present study, we employ density functional theory calculations with the Hubbard U correction (DFT+U) to explore the structural and electronic characteristics of La-doped TiO 2 and two structural variants co-doped with La and Mg. In one of the two co-doped materials, La and Mg atoms replace O and Ti, respectively (TiO 2 -La (1) -Mg (1) ), while in the other, La and Mg substitute for two Ti atoms (TiO 2 -La (2) -Mg (1) ). The singularly La-doped material, TiO 2 -La (3) , is formed by replacing one Ti atom with an La atom. Our comprehensive analysis, formation energy and Koopman's calculations, aimed to determine structural stability. The results indicate that under O-rich or Ti-rich conditions, TiO 2 -La (2) -Mg (1) shows the most promising characteristics. Assessment of the electronic structure reveals that TiO 2 -La (2) -Mg (1) and TiO 2 -La (3) have a lower density of trap states compared to TiO 2 -La (1) -Mg (1) . Analysis of the optical spectrum indicates that TiO 2 -La (2) -Mg (1) exhibits the highest absorption ability in visible range, closely followed by TiO 2 -La (1) -Mg (1) and TiO 2 -La (3) , respectively. In conclusion TiO 2 -La (2) -Mg (1) and TiO 2 -La (3) are identified as the most promising structures, emphasizing the importance of striking a balance between trap states and a narrowed band gap to achieve optimal performance. Furthermore, our findings suggest the potential for efficient TiO 2 co-doped structures under specific growth conditions, highlighting a novel avenue for exploration in both theoretical and experimental domains. • TiO 2 -La (2) -Mg (1) emerges as the most promising ETL material. • La substitution to TiO 2 introduces significant trap states. • For better ETL, trap state has to be fine tune with band gap. • La-Mg dope TiO 2 performance could enhance by applying O-rich or Ti-rich growth condition during synthesizing.

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Publication Details

Journal
Journal of Physics and Chemistry of Solids
Published
2025-07-05
DOI
https://doi.org/10.1016/j.jpcs.2025.113004
Citations
2
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
1.46
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article

First-principles study of La and Mg doped/co-doped TiO2 for tailoring trap states in the electron transport layer of perovskite solar cells

Roshan Thotagamuge, Yashas Balasooriya, Piyasiri Ekanayake, James R. Jennings et al.
2 citations
Journal of Physics and Chemistry of Solids
Perovskite Materials and Applications
1.46
article

First-principles study of La and Mg doped/co-doped TiO2 for tailoring trap states in the electron transport layer of perovskite solar cells

Roshan Thotagamuge, Yashas Balasooriya, Piyasiri Ekanayake, James R. Jennings, Narayan Prasad Adhikari
article en
2 citations

Abstract

Doping TiO 2 with La and Mg shows promise in enhancing its performance as an electron transport layer (ETL) in perovskite solar cells. Yet, a comprehensive understanding of the specific contributions of these dopants to TiO 2 properties remains elusive. In the present study, we employ density functional theory calculations with the Hubbard U correction (DFT+U) to explore the structural and electronic characteristics of La-doped TiO 2 and two structural variants co-doped with La and Mg. In one of the two co-doped materials, La and Mg atoms replace O and Ti, respectively (TiO 2 -La (1) -Mg (1) ), while in the other, La and Mg substitute for two Ti atoms (TiO 2 -La (2) -Mg (1) ). The singularly La-doped material, TiO 2 -La (3) , is formed by replacing one Ti atom with an La atom. Our comprehensive analysis, formation energy and Koopman's calculations, aimed to determine structural stability. The results indicate that under O-rich or Ti-rich conditions, TiO 2 -La (2) -Mg (1) shows the most promising characteristics. Assessment of the electronic structure reveals that TiO 2 -La (2) -Mg (1) and TiO 2 -La (3) have a lower density of trap states compared to TiO 2 -La (1) -Mg (1) . Analysis of the optical spectrum indicates that TiO 2 -La (2) -Mg (1) exhibits the highest absorption ability in visible range, closely followed by TiO 2 -La (1) -Mg (1) and TiO 2 -La (3) , respectively. In conclusion TiO 2 -La (2) -Mg (1) and TiO 2 -La (3) are identified as the most promising structures, emphasizing the importance of striking a balance between trap states and a narrowed band gap to achieve optimal performance. Furthermore, our findings suggest the potential for efficient TiO 2 co-doped structures under specific growth conditions, highlighting a novel avenue for exploration in both theoretical and experimental domains. • TiO 2 -La (2) -Mg (1) emerges as the most promising ETL material. • La substitution to TiO 2 introduces significant trap states. • For better ETL, trap state has to be fine tune with band gap. • La-Mg dope TiO 2 performance could enhance by applying O-rich or Ti-rich growth condition during synthesizing.

Journal of Physics and Chemistry of SolidsVol. 208
University of Kansas (US), Tribhuvan University (NP), Wayamba University of Sri Lanka (LK), Universiti Brunei Darussalam (BN)
Affordable and clean energy
Openalex Percentile: Top 16%
Perovskite Materials and Applications
1.46
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