Structural and Optoelectronic Properties of Two-Dimensional Ruddlesden–Popper Hybrid Perovskite CsSnBr<sub>3</sub>

Ultrathin inorganic halogenated perovskites have attracted attention owing to their excellent photoelectric properties. In this work, we designed two types of Ruddlesden–Popper hybrid perovskites, Cs<i><sub>n</sub></i><sub>+1</sub>Sn<i><sub>n</sub&g...

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Main Authors: Guangbiao Xiang, Yanwen Wu, Yushuang Li, Chen Cheng, Jiancai Leng, Hong Ma
Format: Article
Language:English
Published: MDPI AG 2021-08-01
Series:Nanomaterials
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Online Access:https://www.mdpi.com/2079-4991/11/8/2119
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spelling doaj-2ef381c5846b43e3898d16f4e5cd37aa2021-08-26T14:09:34ZengMDPI AGNanomaterials2079-49912021-08-01112119211910.3390/nano11082119Structural and Optoelectronic Properties of Two-Dimensional Ruddlesden–Popper Hybrid Perovskite CsSnBr<sub>3</sub>Guangbiao Xiang0Yanwen Wu1Yushuang Li2Chen Cheng3Jiancai Leng4Hong Ma5Shandong Provincial Key Laboratory of Optics, Photonic Device and Collaborative Innovation Center of Light Manipulations and Applications, School of Physics and Electronics, Shandong Normal University, Jinan 250014, ChinaShandong Provincial Key Laboratory of Optics, Photonic Device and Collaborative Innovation Center of Light Manipulations and Applications, School of Physics and Electronics, Shandong Normal University, Jinan 250014, ChinaShandong Provincial Key Laboratory of Optics, Photonic Device and Collaborative Innovation Center of Light Manipulations and Applications, School of Physics and Electronics, Shandong Normal University, Jinan 250014, ChinaShandong Provincial Key Laboratory of Optics, Photonic Device and Collaborative Innovation Center of Light Manipulations and Applications, School of Physics and Electronics, Shandong Normal University, Jinan 250014, ChinaSchool of Electronic and Information Engineering (Department of Physics), Qilu University of Technology (Shandong Academy of Sciences), Jinan 250353, ChinaShandong Provincial Key Laboratory of Optics, Photonic Device and Collaborative Innovation Center of Light Manipulations and Applications, School of Physics and Electronics, Shandong Normal University, Jinan 250014, ChinaUltrathin inorganic halogenated perovskites have attracted attention owing to their excellent photoelectric properties. In this work, we designed two types of Ruddlesden–Popper hybrid perovskites, Cs<i><sub>n</sub></i><sub>+1</sub>Sn<i><sub>n</sub></i>Br<sub>3<i>n</i>+1</sub> and Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub>, and studied their band structures and band gaps as a function of the number of layers (<i>n</i> = 1–5). The calculation results show that Cs<i><sub>n+</sub></i><sub>1</sub>Sn<i><sub>n</sub></i>Br<sub>3<i>n</i>+1</sub> has a direct bandgap while the bandgap of Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub> can be altered from indirect to direct, induced by the 5<i>p</i>-Sn state. As the layers increased from 1 to 5, the bandgap energies of Cs<i><sub>n</sub></i><sub>+1</sub>Sn<i><sub>n</sub></i>Br<sub>3<i>n</i>+1</sub> and Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub> decreased from 1.209 to 0.797 eV and 1.310 to 1.013 eV, respectively. In addition, the optical absorption of Cs<i><sub>n</sub></i><sub>+1</sub>Sn<i><sub>n</sub></i>Br<sub>3<i>n</i>+1</sub> and Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub> was blue-shifted as the structure changed from bulk to nanolayer. Compared with that of Cs<i><sub>n+</sub></i><sub>1</sub>Sn<sub>n</sub>Br<sub>3<i>n+</i>1</sub>, the optical absorption of Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub> was sensitive to the layers along the <i>z</i> direction, which exhibited anisotropy induced by the SnBr<sub>2</sub>-terminated surface.https://www.mdpi.com/2079-4991/11/8/21192D Ruddlesden–Popper hybrid perovskitesfirst-principles studyband structuresoptoelectronic properties
collection DOAJ
language English
format Article
sources DOAJ
author Guangbiao Xiang
Yanwen Wu
Yushuang Li
Chen Cheng
Jiancai Leng
Hong Ma
spellingShingle Guangbiao Xiang
Yanwen Wu
Yushuang Li
Chen Cheng
Jiancai Leng
Hong Ma
Structural and Optoelectronic Properties of Two-Dimensional Ruddlesden–Popper Hybrid Perovskite CsSnBr<sub>3</sub>
Nanomaterials
2D Ruddlesden–Popper hybrid perovskites
first-principles study
band structures
optoelectronic properties
author_facet Guangbiao Xiang
Yanwen Wu
Yushuang Li
Chen Cheng
Jiancai Leng
Hong Ma
author_sort Guangbiao Xiang
title Structural and Optoelectronic Properties of Two-Dimensional Ruddlesden–Popper Hybrid Perovskite CsSnBr<sub>3</sub>
title_short Structural and Optoelectronic Properties of Two-Dimensional Ruddlesden–Popper Hybrid Perovskite CsSnBr<sub>3</sub>
title_full Structural and Optoelectronic Properties of Two-Dimensional Ruddlesden–Popper Hybrid Perovskite CsSnBr<sub>3</sub>
title_fullStr Structural and Optoelectronic Properties of Two-Dimensional Ruddlesden–Popper Hybrid Perovskite CsSnBr<sub>3</sub>
title_full_unstemmed Structural and Optoelectronic Properties of Two-Dimensional Ruddlesden–Popper Hybrid Perovskite CsSnBr<sub>3</sub>
title_sort structural and optoelectronic properties of two-dimensional ruddlesden–popper hybrid perovskite cssnbr<sub>3</sub>
publisher MDPI AG
series Nanomaterials
issn 2079-4991
publishDate 2021-08-01
description Ultrathin inorganic halogenated perovskites have attracted attention owing to their excellent photoelectric properties. In this work, we designed two types of Ruddlesden–Popper hybrid perovskites, Cs<i><sub>n</sub></i><sub>+1</sub>Sn<i><sub>n</sub></i>Br<sub>3<i>n</i>+1</sub> and Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub>, and studied their band structures and band gaps as a function of the number of layers (<i>n</i> = 1–5). The calculation results show that Cs<i><sub>n+</sub></i><sub>1</sub>Sn<i><sub>n</sub></i>Br<sub>3<i>n</i>+1</sub> has a direct bandgap while the bandgap of Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub> can be altered from indirect to direct, induced by the 5<i>p</i>-Sn state. As the layers increased from 1 to 5, the bandgap energies of Cs<i><sub>n</sub></i><sub>+1</sub>Sn<i><sub>n</sub></i>Br<sub>3<i>n</i>+1</sub> and Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub> decreased from 1.209 to 0.797 eV and 1.310 to 1.013 eV, respectively. In addition, the optical absorption of Cs<i><sub>n</sub></i><sub>+1</sub>Sn<i><sub>n</sub></i>Br<sub>3<i>n</i>+1</sub> and Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub> was blue-shifted as the structure changed from bulk to nanolayer. Compared with that of Cs<i><sub>n+</sub></i><sub>1</sub>Sn<sub>n</sub>Br<sub>3<i>n+</i>1</sub>, the optical absorption of Cs<i><sub>n</sub></i>Sn<i><sub>n</sub></i><sub>+1</sub>Br<sub>3<i>n</i>+2</sub> was sensitive to the layers along the <i>z</i> direction, which exhibited anisotropy induced by the SnBr<sub>2</sub>-terminated surface.
topic 2D Ruddlesden–Popper hybrid perovskites
first-principles study
band structures
optoelectronic properties
url https://www.mdpi.com/2079-4991/11/8/2119
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