Unusual Temperature Dependence of Bandgap in 2D Inorganic Lead‐Halide Perovskite Nanoplatelets
Abstract Understanding the origin of temperature‐dependent bandgap in inorganic lead‐halide perovskites is essential and important for their applications in photovoltaics and optoelectronics. Herein, it is found that the temperature dependence of bandgap in CsPbBr3 perovskites is variable with mater...
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doaj-0d0eff5d7816488a8090cea4aae4889a2021-10-08T09:03:06ZengWileyAdvanced Science2198-38442021-10-01819n/an/a10.1002/advs.202100084Unusual Temperature Dependence of Bandgap in 2D Inorganic Lead‐Halide Perovskite NanoplateletsShaohua Yu0Jin Xu1Xiaoying Shang2En Ma3Fulin Lin4Wei Zheng5Datao Tu6Renfu Li7Xueyuan Chen8CAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaCAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaCAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaCAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaCAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaCAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaCAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaCAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaCAS Key Laboratory of Design and Assembly of Functional Nanostructures State Key Laboratory of Structural Chemistry and Fujian Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou Fujian 350002 ChinaAbstract Understanding the origin of temperature‐dependent bandgap in inorganic lead‐halide perovskites is essential and important for their applications in photovoltaics and optoelectronics. Herein, it is found that the temperature dependence of bandgap in CsPbBr3 perovskites is variable with material dimensionality. In contrast to the monotonous redshift ordinarily observed in bulk‐like CsPbBr3 nanocrystals (NCs), the bandgap of 2D CsPbBr3 nanoplatelets (NPLs) exhibits an initial blueshift then redshift trend with decreasing temperature (290–10 K). The Bose–Einstein two‐oscillator modeling manifests that the blueshift‐redshift crossover of bandgap in the NPLs is attributed to the significantly larger weight of contribution from electron‐optical phonon interaction to the bandgap renormalization in the NPLs than in the NCs. These new findings may gain deep insights into the origin of bandgap shift with temperature for both fundamentals and applications of perovskite semiconductor materials.https://doi.org/10.1002/advs.202100084blueshift‐redshift crossoverinorganic lead‐halide perovskitesmaterial dimensionalitytemperature‐dependent bandgap |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Shaohua Yu Jin Xu Xiaoying Shang En Ma Fulin Lin Wei Zheng Datao Tu Renfu Li Xueyuan Chen |
spellingShingle |
Shaohua Yu Jin Xu Xiaoying Shang En Ma Fulin Lin Wei Zheng Datao Tu Renfu Li Xueyuan Chen Unusual Temperature Dependence of Bandgap in 2D Inorganic Lead‐Halide Perovskite Nanoplatelets Advanced Science blueshift‐redshift crossover inorganic lead‐halide perovskites material dimensionality temperature‐dependent bandgap |
author_facet |
Shaohua Yu Jin Xu Xiaoying Shang En Ma Fulin Lin Wei Zheng Datao Tu Renfu Li Xueyuan Chen |
author_sort |
Shaohua Yu |
title |
Unusual Temperature Dependence of Bandgap in 2D Inorganic Lead‐Halide Perovskite Nanoplatelets |
title_short |
Unusual Temperature Dependence of Bandgap in 2D Inorganic Lead‐Halide Perovskite Nanoplatelets |
title_full |
Unusual Temperature Dependence of Bandgap in 2D Inorganic Lead‐Halide Perovskite Nanoplatelets |
title_fullStr |
Unusual Temperature Dependence of Bandgap in 2D Inorganic Lead‐Halide Perovskite Nanoplatelets |
title_full_unstemmed |
Unusual Temperature Dependence of Bandgap in 2D Inorganic Lead‐Halide Perovskite Nanoplatelets |
title_sort |
unusual temperature dependence of bandgap in 2d inorganic lead‐halide perovskite nanoplatelets |
publisher |
Wiley |
series |
Advanced Science |
issn |
2198-3844 |
publishDate |
2021-10-01 |
description |
Abstract Understanding the origin of temperature‐dependent bandgap in inorganic lead‐halide perovskites is essential and important for their applications in photovoltaics and optoelectronics. Herein, it is found that the temperature dependence of bandgap in CsPbBr3 perovskites is variable with material dimensionality. In contrast to the monotonous redshift ordinarily observed in bulk‐like CsPbBr3 nanocrystals (NCs), the bandgap of 2D CsPbBr3 nanoplatelets (NPLs) exhibits an initial blueshift then redshift trend with decreasing temperature (290–10 K). The Bose–Einstein two‐oscillator modeling manifests that the blueshift‐redshift crossover of bandgap in the NPLs is attributed to the significantly larger weight of contribution from electron‐optical phonon interaction to the bandgap renormalization in the NPLs than in the NCs. These new findings may gain deep insights into the origin of bandgap shift with temperature for both fundamentals and applications of perovskite semiconductor materials. |
topic |
blueshift‐redshift crossover inorganic lead‐halide perovskites material dimensionality temperature‐dependent bandgap |
url |
https://doi.org/10.1002/advs.202100084 |
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