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Temperature-Dependent Photoluminescence of Manganese Halide with Tetrahedron Structure in Anti-Perovskites

The temperature-dependent photoluminescence (PL) properties of an anti-perovskite [MnBr(4)]BrCs(3) sample in the temperature range of 78–500 K are studied in the present work. This material exhibits unique performance which is different from a typical perovskite. Experiments showed that from room te...

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Autores principales: Xia, Yijie, Du, Shuaishuai, Huang, Pengju, Wu, Luchao, Yan, Siyu, Wang, Weizhi, Zhong, Gaoyu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8706729/
https://www.ncbi.nlm.nih.gov/pubmed/34947660
http://dx.doi.org/10.3390/nano11123310
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author Xia, Yijie
Du, Shuaishuai
Huang, Pengju
Wu, Luchao
Yan, Siyu
Wang, Weizhi
Zhong, Gaoyu
author_facet Xia, Yijie
Du, Shuaishuai
Huang, Pengju
Wu, Luchao
Yan, Siyu
Wang, Weizhi
Zhong, Gaoyu
author_sort Xia, Yijie
collection PubMed
description The temperature-dependent photoluminescence (PL) properties of an anti-perovskite [MnBr(4)]BrCs(3) sample in the temperature range of 78–500 K are studied in the present work. This material exhibits unique performance which is different from a typical perovskite. Experiments showed that from room temperature to 78 K, the luminous intensity increased as the temperature decreased. From room temperature to 500 K, the photoluminescence intensity gradually decreased with increasing temperature. Experiments with varying temperatures repeatedly showed that the emission wavelength was very stable. Based on the above-mentioned phenomenon of the changing photoluminescence under different temperatures, the mechanism is deduced from the temperature-dependent characteristics of excitons, and the experimental results are explained on the basis of the types of excitons with different energy levels and different recombination rates involved in the steady-state PL process. The results show that in the measured temperature range of 78–500 K, the steady-state PL of [MnBr(4)]BrCs(3) had three excitons with different energy levels and recombination rates participating. The involved excitons with the highest energy level not only had a high radiative recombination rate, but a high non-radiative recombination rate as well. The excitons at the second-highest energy level had a similar radiative recombination rate to the lowest energy level excitons and a had high non-radiative recombination rate. These excitons made the photoluminescence gradually decrease with increasing temperature. This may be the reason for this material’s high photoluminescence efficiency and low electroluminescence efficiency.
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spelling pubmed-87067292021-12-25 Temperature-Dependent Photoluminescence of Manganese Halide with Tetrahedron Structure in Anti-Perovskites Xia, Yijie Du, Shuaishuai Huang, Pengju Wu, Luchao Yan, Siyu Wang, Weizhi Zhong, Gaoyu Nanomaterials (Basel) Article The temperature-dependent photoluminescence (PL) properties of an anti-perovskite [MnBr(4)]BrCs(3) sample in the temperature range of 78–500 K are studied in the present work. This material exhibits unique performance which is different from a typical perovskite. Experiments showed that from room temperature to 78 K, the luminous intensity increased as the temperature decreased. From room temperature to 500 K, the photoluminescence intensity gradually decreased with increasing temperature. Experiments with varying temperatures repeatedly showed that the emission wavelength was very stable. Based on the above-mentioned phenomenon of the changing photoluminescence under different temperatures, the mechanism is deduced from the temperature-dependent characteristics of excitons, and the experimental results are explained on the basis of the types of excitons with different energy levels and different recombination rates involved in the steady-state PL process. The results show that in the measured temperature range of 78–500 K, the steady-state PL of [MnBr(4)]BrCs(3) had three excitons with different energy levels and recombination rates participating. The involved excitons with the highest energy level not only had a high radiative recombination rate, but a high non-radiative recombination rate as well. The excitons at the second-highest energy level had a similar radiative recombination rate to the lowest energy level excitons and a had high non-radiative recombination rate. These excitons made the photoluminescence gradually decrease with increasing temperature. This may be the reason for this material’s high photoluminescence efficiency and low electroluminescence efficiency. MDPI 2021-12-06 /pmc/articles/PMC8706729/ /pubmed/34947660 http://dx.doi.org/10.3390/nano11123310 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Xia, Yijie
Du, Shuaishuai
Huang, Pengju
Wu, Luchao
Yan, Siyu
Wang, Weizhi
Zhong, Gaoyu
Temperature-Dependent Photoluminescence of Manganese Halide with Tetrahedron Structure in Anti-Perovskites
title Temperature-Dependent Photoluminescence of Manganese Halide with Tetrahedron Structure in Anti-Perovskites
title_full Temperature-Dependent Photoluminescence of Manganese Halide with Tetrahedron Structure in Anti-Perovskites
title_fullStr Temperature-Dependent Photoluminescence of Manganese Halide with Tetrahedron Structure in Anti-Perovskites
title_full_unstemmed Temperature-Dependent Photoluminescence of Manganese Halide with Tetrahedron Structure in Anti-Perovskites
title_short Temperature-Dependent Photoluminescence of Manganese Halide with Tetrahedron Structure in Anti-Perovskites
title_sort temperature-dependent photoluminescence of manganese halide with tetrahedron structure in anti-perovskites
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8706729/
https://www.ncbi.nlm.nih.gov/pubmed/34947660
http://dx.doi.org/10.3390/nano11123310
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