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Liu D, Zeng H, Peng H, Sa R. A theoretical exploration of the structural feature, mechanical, and optoelectronic properties of Au-based halide perovskites A 2Au IAu IIIX 6 (A = Rb, Cs; X = Cl, Br, I). Phys Chem Chem Phys 2023; 25:28974-28981. [PMID: 37859496 DOI: 10.1039/d3cp04269c] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/21/2023]
Abstract
As a possible alternative to lead halide perovskites, inorganic mixed-valence Au-based halide perovskites have drawn much attention. In the current research, we have conducted comprehensive theoretical calculations to reveal the structural feature, thermodynamic and dynamic stability, mechanical behavior, optoelectronic properties, and photovoltaic performance of Au-based halide perovskites A2AuIAuIIIX6 (A = Rb, Cs; X = Cl, Br, I). The structural parameters of these compounds are carefully analyzed. Our calculations indicate that the thermodynamic, dynamic, and mechanical stability of monoclinic Rb2AuIAuIIIX6 and tetragonal Cs2AuIAuIIIX6 are ensured, and they are all ductile. The electronic band structure analysis shows that Rb2AuIAuIIII6 illustrates a direct-gap feature, while Rb2AuIAuIIIX6 (X = Cl, Br) and Cs2AuIAuIIIX6 (X = Cl, Br, I) are indirect-gap materials. The effect of A-site cation substitution on the optical band gaps of the Au-based halide perovskites is elucidated. Our results further suggest that Rb2AuIAuIIIX6 (X = Br, I) and Cs2AuIAuIIIX6 (X = Cl, Br, I) are more suitable for single-junction solar cells due to their suitable band gaps within 1.1-1.5 eV. Furthermore, four compounds A2AuIAuIIIX6 (A = Rb, Cs; X = Br, I) not only have high absorption coefficients in the visible region but also show excellent photovoltaic performance, especially for A2AuIAuIIII6 (A = Rb, Cs), whose efficiency can reach over 29% with a film thickness of 0.5 μm. Our study suggests that inorganic Au-based halide perovskites are potential alternatives for optoelectronic devices in solar cells.
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Affiliation(s)
- Diwen Liu
- School of Materials and Chemical Engineering, Pingxiang University, Pingxiang, 337055, China.
| | - Huihui Zeng
- School of Materials and Chemical Engineering, Pingxiang University, Pingxiang, 337055, China.
| | - Huan Peng
- School of Materials and Chemical Engineering, Pingxiang University, Pingxiang, 337055, China.
| | - Rongjian Sa
- College of Materials and Chemical Engineering, Minjiang University, Fuzhou, 350108, China.
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Chen Y, Ding X, Yang L, Wang Y, Gurti JI, Wang M, Li W, Wang X, Yang W. Small practical cluster models for perovskites based on the similarity criterion of central location environment and their applications. Phys Chem Chem Phys 2022; 24:14375-14389. [PMID: 35642957 DOI: 10.1039/d2cp00562j] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/21/2022]
Abstract
Developing universal theoretical models for perovskites (often denoted as ABX3) can contribute to the rational design of novel perovskite photovoltaic materials. However, few models can be successfully applied to study the intrinsic electronic structure due to the poor accuracy and unaffordable computational cost. Herein, we report the innovative construction of small practical cluster models through the similarity criterion of the central location environment, which retains only the central A-site as the original cation while the others are substituted by Cs to keep the clusters electrically neutral. The central cation has a chemical environment similar to that of the bulk perovskite. The binding energy between A and the BX framework, geometric structures (B-X distances and B-X-B angles), and the electronic structures (the gap and the spatial distribution of HOMO and LUMO, electron distribution) of these clusters have been investigated and compared with the corresponding properties of bulk materials. The results suggest that the cluster model with twelve B-atoms suitably describes these properties. The geometric structures and gaps are closer to the bulk situations than the quasi-one-dimensional and quasi-two-dimensional cluster models with all-primitive cations, respectively. Other organic cations, such as NH3(CH2)nCH3 (n = 1, 2, and 3 for EA, PA, and BA, respectively), and (NH2)2CH (FA) can, therefore, mimic perovskite materials. Clusters with different sizes of A indicate that PA and BA will distort the quasi-cubic structures, which is consistent with the judgment of the tolerance factor of bulk materials. The reliable cluster model provides the research foundation for some basic issues of perovskites, such as vibrational spectroscopy and hydrogen bonding strength, to gain detailed insight into the interactions between A and the BX framework.
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Affiliation(s)
- Yan Chen
- School of Mathematics and Physics, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China. .,School of New Energy, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China
| | - Xunlei Ding
- School of Mathematics and Physics, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China. .,Institute of Clusters and Low Dimensional Nanomaterials, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China
| | - Luona Yang
- School of Mathematics and Physics, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China. .,Institute of Clusters and Low Dimensional Nanomaterials, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China
| | - Yaya Wang
- School of Mathematics and Physics, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China. .,School of New Energy, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China
| | - Joseph Israel Gurti
- School of Mathematics and Physics, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China. .,Institute of Clusters and Low Dimensional Nanomaterials, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China
| | - Mengmeng Wang
- School of Mathematics and Physics, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China. .,School of New Energy, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China
| | - Wei Li
- School of Mathematics and Physics, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China. .,Institute of Clusters and Low Dimensional Nanomaterials, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China
| | - Xin Wang
- School of Mathematics and Physics, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China. .,Institute of Clusters and Low Dimensional Nanomaterials, North China Electric Power University, Beinong Road 2, Huilongguan, Beijing 102206, P. R. China
| | - Weijie Yang
- Department of Power Engineering, School of Energy, Power and Mechanical Engineering, North China Electric Power University, Baoding 071003, China.
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