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Dimensional reduction of the small-bandgap double perovskite Cs(2)AgTlBr(6)
Quantum confinement effects in lower-dimensional derivatives of the ABX(3) (A = monocation, X = halide) single perovskites afford striking optical and electronic changes, enabling applications ranging from solar absorbers to phosphors and light-emitting diodes. Halide double perovskites form a large...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Royal Society of Chemistry
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7450713/ https://www.ncbi.nlm.nih.gov/pubmed/32874527 http://dx.doi.org/10.1039/d0sc01580f |
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author | Connor, Bridget A. Biega, Raisa-Ioana Leppert, Linn Karunadasa, Hemamala I. |
author_facet | Connor, Bridget A. Biega, Raisa-Ioana Leppert, Linn Karunadasa, Hemamala I. |
author_sort | Connor, Bridget A. |
collection | PubMed |
description | Quantum confinement effects in lower-dimensional derivatives of the ABX(3) (A = monocation, X = halide) single perovskites afford striking optical and electronic changes, enabling applications ranging from solar absorbers to phosphors and light-emitting diodes. Halide double perovskites form a larger materials family, known since the late 1800s, but lower-dimensional derivatives remain rare and prior work has revealed a minimal effect of quantum confinement on their optical properties. Here, we synthesize three new lower-dimensional derivatives of the 3D double perovskite Cs(2)AgTlBr(6): 2D derivatives with mono- (1-Tl) and bi-layer thick (2-Tl) inorganic sheets and a quasi-1D derivative (1'-Tl). Single-crystal ellipsometry studies of these materials show the first clear demonstration that dimensional reduction can significantly alter the optical properties of 2D halide double perovskites. This large quantum confinement effect is attributed to the substantial electronic delocalization of the parent 3D Ag–Tl perovskite. Calculations track the evolution of the electronic bands with dimensional reduction and the accompanying structural distortions and show a direct-to-indirect bandgap transition as the 3D perovskite lattice is thinned to a monolayer in 1-Tl. This bandgap transition at the monolayer limit is also evident in the calculations for 1-In, an isostructural, isoelectronic analogue to 1-Tl in which In(3+) replaces Tl(3+), underscoring the orbital basis for the direct/indirect nature of the bandgap. Thus, in complement to the massive compositional diversity of halide double perovskites, dimensional reduction may be used as a systematic route for harnessing electronic confinement effects and obtaining new electronic structures. |
format | Online Article Text |
id | pubmed-7450713 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-74507132020-08-31 Dimensional reduction of the small-bandgap double perovskite Cs(2)AgTlBr(6) Connor, Bridget A. Biega, Raisa-Ioana Leppert, Linn Karunadasa, Hemamala I. Chem Sci Chemistry Quantum confinement effects in lower-dimensional derivatives of the ABX(3) (A = monocation, X = halide) single perovskites afford striking optical and electronic changes, enabling applications ranging from solar absorbers to phosphors and light-emitting diodes. Halide double perovskites form a larger materials family, known since the late 1800s, but lower-dimensional derivatives remain rare and prior work has revealed a minimal effect of quantum confinement on their optical properties. Here, we synthesize three new lower-dimensional derivatives of the 3D double perovskite Cs(2)AgTlBr(6): 2D derivatives with mono- (1-Tl) and bi-layer thick (2-Tl) inorganic sheets and a quasi-1D derivative (1'-Tl). Single-crystal ellipsometry studies of these materials show the first clear demonstration that dimensional reduction can significantly alter the optical properties of 2D halide double perovskites. This large quantum confinement effect is attributed to the substantial electronic delocalization of the parent 3D Ag–Tl perovskite. Calculations track the evolution of the electronic bands with dimensional reduction and the accompanying structural distortions and show a direct-to-indirect bandgap transition as the 3D perovskite lattice is thinned to a monolayer in 1-Tl. This bandgap transition at the monolayer limit is also evident in the calculations for 1-In, an isostructural, isoelectronic analogue to 1-Tl in which In(3+) replaces Tl(3+), underscoring the orbital basis for the direct/indirect nature of the bandgap. Thus, in complement to the massive compositional diversity of halide double perovskites, dimensional reduction may be used as a systematic route for harnessing electronic confinement effects and obtaining new electronic structures. Royal Society of Chemistry 2020-06-05 /pmc/articles/PMC7450713/ /pubmed/32874527 http://dx.doi.org/10.1039/d0sc01580f Text en This journal is © The Royal Society of Chemistry 2020 http://creativecommons.org/licenses/by-nc/3.0/ This article is freely available. This article is licensed under a Creative Commons Attribution Non Commercial 3.0 Unported Licence (CC BY-NC 3.0) |
spellingShingle | Chemistry Connor, Bridget A. Biega, Raisa-Ioana Leppert, Linn Karunadasa, Hemamala I. Dimensional reduction of the small-bandgap double perovskite Cs(2)AgTlBr(6) |
title | Dimensional reduction of the small-bandgap double perovskite Cs(2)AgTlBr(6)
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title_full | Dimensional reduction of the small-bandgap double perovskite Cs(2)AgTlBr(6)
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title_fullStr | Dimensional reduction of the small-bandgap double perovskite Cs(2)AgTlBr(6)
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title_full_unstemmed | Dimensional reduction of the small-bandgap double perovskite Cs(2)AgTlBr(6)
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title_short | Dimensional reduction of the small-bandgap double perovskite Cs(2)AgTlBr(6)
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title_sort | dimensional reduction of the small-bandgap double perovskite cs(2)agtlbr(6) |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7450713/ https://www.ncbi.nlm.nih.gov/pubmed/32874527 http://dx.doi.org/10.1039/d0sc01580f |
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