High-Contrast Thermochromism in Room-Temperature Transparent Layered Perovskite PEA<sub>2</sub>PbBr<sub>4</sub> with a High Temperature-Induced Bandgap Change Rate of 0.8 meV/K

Two-dimensional organic-inorganic hybrid layered perovskites have emerged as a new generation of optoelectronic materials. However, the thermochromism in organic-inorganic hybrid layered perovskites has been rarely explored in depth. A further understanding of the mechanism is necessary and favorable for the application. Here, transparent centimeter-sized single crystals of the organic-inorganic hybrid layered perovskite (C<sub>6</sub>H<sub>5</sub>C<sub>2</sub>H<sub>4</sub>NH<sub>3</sub>)<sub>2</sub>PbBr<sub>4</sub> (PEA<sub>2</sub>PbBr<sub>4</sub>) were synthesized using an improved evaporation method. As a typical organic-inorganic hybrid layered perovskite, the PEA<sub>2</sub>PbBr<sub>4</sub> single crystal shows high-contrast and progressive thermochromism exhibiting a change from colorlessness and transparency to lemon yellow in a wide temperature range of 200-450 K. Based on the calculation through the Varshni equation, the temperature-induced bandgap change rate directly associated with the high-contrast thermochromism of PEA<sub>2</sub>PbBr<sub>4</sub> reaching 0.8 meV/K. This value is higher than that of many three-dimensional perovskites and traditional IV-III semiconductors. Furthermore, the temperature-dependent 193 nm photoluminescence spectra suggest that this high temperature-induced bandgap change rate of PEA<sub>2</sub>PbBr<sub>4</sub> is a result of the competitive interaction between lattice thermal expansion and electron-phonon coupling (Fröhlich coupling coefficient Γ<sub>LO</sub> = 2.215). Based on the characteristics introduced above, PEA<sub>2</sub>PbBr<sub>4</sub> as an organic-inorganic hybrid layered perovskite has a better performance in achieving the balance between high-contrast and high room-temperature transmittance. Therefore, PEA<sub>2</sub>PbBr<sub>4</sub> is a material with great potential in applications like temperature-indicating labels. This work provides valuable insights into the thermochromism of layered perovskites, offering a new material system and approach for developing thermochromic materials with higher sensitivity and efficiency.

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Publication Details

Journal
Journal of the American Chemical Society
Published
2024-08-21
DOI
https://doi.org/10.1021/jacs.4c09090
Citations
22
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
4.59

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article

High-Contrast Thermochromism in Room-Temperature Transparent Layered Perovskite PEA2PbBr4 with a High Temperature-Induced Bandgap Change Rate of 0.8 meV/K

Danwen Zhang, Wei Zheng, Xiaoyu Song, Siqi Zhu et al.
22 citations
Journal of the American Chemical Society
Perovskite Materials and Applications
4.59
article

High-Contrast Thermochromism in Room-Temperature Transparent Layered Perovskite PEA2PbBr4 with a High Temperature-Induced Bandgap Change Rate of 0.8 meV/K

Danwen Zhang, Wei Zheng, Xiaoyu Song, Siqi Zhu, Xinsheng Liu, Jingyan Liao
article en
22 citations

Abstract

Two-dimensional organic-inorganic hybrid layered perovskites have emerged as a new generation of optoelectronic materials. However, the thermochromism in organic-inorganic hybrid layered perovskites has been rarely explored in depth. A further understanding of the mechanism is necessary and favorable for the application. Here, transparent centimeter-sized single crystals of the organic-inorganic hybrid layered perovskite (C<sub>6</sub>H<sub>5</sub>C<sub>2</sub>H<sub>4</sub>NH<sub>3</sub>)<sub>2</sub>PbBr<sub>4</sub> (PEA<sub>2</sub>PbBr<sub>4</sub>) were synthesized using an improved evaporation method. As a typical organic-inorganic hybrid layered perovskite, the PEA<sub>2</sub>PbBr<sub>4</sub> single crystal shows high-contrast and progressive thermochromism exhibiting a change from colorlessness and transparency to lemon yellow in a wide temperature range of 200-450 K. Based on the calculation through the Varshni equation, the temperature-induced bandgap change rate directly associated with the high-contrast thermochromism of PEA<sub>2</sub>PbBr<sub>4</sub> reaching 0.8 meV/K. This value is higher than that of many three-dimensional perovskites and traditional IV-III semiconductors. Furthermore, the temperature-dependent 193 nm photoluminescence spectra suggest that this high temperature-induced bandgap change rate of PEA<sub>2</sub>PbBr<sub>4</sub> is a result of the competitive interaction between lattice thermal expansion and electron-phonon coupling (Fröhlich coupling coefficient Γ<sub>LO</sub> = 2.215). Based on the characteristics introduced above, PEA<sub>2</sub>PbBr<sub>4</sub> as an organic-inorganic hybrid layered perovskite has a better performance in achieving the balance between high-contrast and high room-temperature transmittance. Therefore, PEA<sub>2</sub>PbBr<sub>4</sub> is a material with great potential in applications like temperature-indicating labels. This work provides valuable insights into the thermochromism of layered perovskites, offering a new material system and approach for developing thermochromic materials with higher sensitivity and efficiency.

Journal of the American Chemical SocietyVol. 146(35)
Sun Yat-sen University (CN)
National Natural Science Foundation of China, Natural Science Foundation of Guangdong Province, National Key Research and Development Program of China
Clean water and sanitation
Openalex Percentile: Top 5%
Perovskite Materials and Applications
4.59
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