Pushing the boundary of the stability and band gap Pareto front by going towards high-entropy perovskites

Lead-free Cs<sub>2</sub>BX<sub>6</sub> (B = Zr<sup>4+</sup>, Sn<sup>4+</sup>, Te<sup>4+</sup>, Hf<sup>4+</sup>, Re<sup>4+</sup>, Os<sup>4+</sup>, Ir<sup>4+</sup>, and Pt<sup>4+</sup> and X = Cl<sup>-</sup>, Br<sup>-</sup>, and I<sup>-</sup>) vacancy-ordered double perovskites have gained significant attention due to their high performance in solar cell devices. Besides mitigating toxicity concerns associated with the use of lead, the presence of a formally tetravalent B-site in Cs<sub>2</sub>BX<sub>6</sub> has been demonstrated to improve the stability against air and moisture. Recently, experimental studies have shown that high-entropy forms of vacancy-ordered double perovskites can be synthesized and stabilized at room temperature, which opens new opportunities for designing better solar cell absorbers. In this work, we employed high throughput density functional theory (DFT) calculations using the HSE06 hybrid functional to study 546 medium-to-high-entropy vacancy-ordered double perovskites. Our results show that Cs<sub>2</sub>{B<sub>1</sub>B<sub>2</sub>B<sub>3</sub>B<sub>4</sub>}<sub>1</sub>X<sub>6</sub> and Cs<sub>2</sub>{B<sub>1</sub>B<sub>2</sub>B<sub>3</sub>B<sub>4</sub>}<sub>1</sub>{XX'}<sub>6</sub> perovskites can break the existing linear scaling relationships between the bandgap and formation energy observed in the pure Cs<sub>2</sub>BX<sub>6</sub> and Cs<sub>2</sub>B{XX'}<sub>6</sub> perovskites, which enables materials that simultaneously exhibit an optimal band gap of ∼1.3 eV for single-junction solar cells along with a low formation energy. Electronic structure analysis reveals that this can be attributed to the weak coupling between the BX<sub>6</sub> octahedra in Cs<sub>2</sub>{B<sub>1</sub>B<sub>2</sub>B<sub>3</sub>B<sub>4</sub>}<sub>1</sub>X<sub>6</sub> and Cs<sub>2</sub>{B<sub>1</sub>B<sub>2</sub>B<sub>3</sub>B<sub>4</sub>}<sub>1</sub>{XX'}<sub>6</sub>. Based on these findings, we identified the analytical equations that can be used to efficiently predict the band gap and formation energy of high-entropy perovskites from their constituent pure perovskites. Our study offers simple and practical guidelines for the design and synthesis of novel high-entropy perovskites with improved photovoltaic performance.

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Publication Details

Journal
Nanoscale
Published
2025-01-01
DOI
https://doi.org/10.1039/d4nr05013d
Citations
2
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
1.46

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article

Pushing the boundary of the stability and band gap Pareto front by going towards high-entropy perovskites

Zhendian Zhang, Victor Fung, Guoxiang Hu
2 citations
Nanoscale
Perovskite Materials and Applications
1.46
article

Pushing the boundary of the stability and band gap Pareto front by going towards high-entropy perovskites

Zhendian Zhang, Victor Fung, Guoxiang Hu
article en
2 citations

Abstract

Lead-free Cs<sub>2</sub>BX<sub>6</sub> (B = Zr<sup>4+</sup>, Sn<sup>4+</sup>, Te<sup>4+</sup>, Hf<sup>4+</sup>, Re<sup>4+</sup>, Os<sup>4+</sup>, Ir<sup>4+</sup>, and Pt<sup>4+</sup> and X = Cl<sup>-</sup>, Br<sup>-</sup>, and I<sup>-</sup>) vacancy-ordered double perovskites have gained significant attention due to their high performance in solar cell devices. Besides mitigating toxicity concerns associated with the use of lead, the presence of a formally tetravalent B-site in Cs<sub>2</sub>BX<sub>6</sub> has been demonstrated to improve the stability against air and moisture. Recently, experimental studies have shown that high-entropy forms of vacancy-ordered double perovskites can be synthesized and stabilized at room temperature, which opens new opportunities for designing better solar cell absorbers. In this work, we employed high throughput density functional theory (DFT) calculations using the HSE06 hybrid functional to study 546 medium-to-high-entropy vacancy-ordered double perovskites. Our results show that Cs<sub>2</sub>{B<sub>1</sub>B<sub>2</sub>B<sub>3</sub>B<sub>4</sub>}<sub>1</sub>X<sub>6</sub> and Cs<sub>2</sub>{B<sub>1</sub>B<sub>2</sub>B<sub>3</sub>B<sub>4</sub>}<sub>1</sub>{XX'}<sub>6</sub> perovskites can break the existing linear scaling relationships between the bandgap and formation energy observed in the pure Cs<sub>2</sub>BX<sub>6</sub> and Cs<sub>2</sub>B{XX'}<sub>6</sub> perovskites, which enables materials that simultaneously exhibit an optimal band gap of ∼1.3 eV for single-junction solar cells along with a low formation energy. Electronic structure analysis reveals that this can be attributed to the weak coupling between the BX<sub>6</sub> octahedra in Cs<sub>2</sub>{B<sub>1</sub>B<sub>2</sub>B<sub>3</sub>B<sub>4</sub>}<sub>1</sub>X<sub>6</sub> and Cs<sub>2</sub>{B<sub>1</sub>B<sub>2</sub>B<sub>3</sub>B<sub>4</sub>}<sub>1</sub>{XX'}<sub>6</sub>. Based on these findings, we identified the analytical equations that can be used to efficiently predict the band gap and formation energy of high-entropy perovskites from their constituent pure perovskites. Our study offers simple and practical guidelines for the design and synthesis of novel high-entropy perovskites with improved photovoltaic performance.

NanoscaleVol. 17(18)
Georgia Institute of Technology (US)
U.S. Department of Energy, National Energy Research Scientific Computing Center, Office of Science
Openalex Percentile: Top 18%
Perovskite Materials and Applications
1.46
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