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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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 |
work_keys_str_mv |
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