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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Main Authors: Shaohua Yu, Jin Xu, Xiaoying Shang, En Ma, Fulin Lin, Wei Zheng, Datao Tu, Renfu Li, Xueyuan Chen
Format: Article
Language:English
Published: Wiley 2021-10-01
Series:Advanced Science
Subjects:
Online Access:https://doi.org/10.1002/advs.202100084
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spelling 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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