Temperature-dependent photoluminescence of lead-free cesium tin halide perovskite microplates

Tin halide perovskites recently have attracted extensive research attention due to their similar electronic and band structures but non-toxicity compared with their lead analogues. In this work, we prepare high-quality CsSn X 3 ( X = Br, I) microplates with lateral sizes of around 1–4 μm by chemical...

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Bibliographic Details
Published in:Chinese physics B 2023-11, Vol.32 (11), p.117802
Main Authors: Tan, Jiayu, Zhou, Yixuan, Lu, De, Feng, Xukun, Liu, Yuqi, Zhang, Mengen, Lu, Fangzhengyi, Huang, Yuanyuan, Xu, Xinlong
Format: Article
Language:English
Subjects:
cesium tin halide perovskite
chemical vapor deposition
microplate
temperature-dependent photoluminescence
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Summary:Tin halide perovskites recently have attracted extensive research attention due to their similar electronic and band structures but non-toxicity compared with their lead analogues. In this work, we prepare high-quality CsSn X 3 ( X = Br, I) microplates with lateral sizes of around 1–4 μm by chemical vapor deposition and investigate their low-temperature photoluminescence (PL) properties. A remarkable splitting of PL peaks of the CsSnBr 3 microplate is observed at low temperatures. Besides the possible structural phase transition at below 70 K, the multi-peak fittings using Gauss functions and the power-dependent saturation phenomenon suggest that the PL could also be influenced by the conversion from the emission of bound excitons into free excitons. With the increase of temperature, the peak position shows a blueshift tendency for CsSnI 3 , which is governed by thermal expansion. However, the peak position of the CsSnBr 3 microplate exhibits a transition from redshift to blueshift at ∼160 K. The full width at half maximum of CsSn X 3 broadens with increasing temperature, and the fitting results imply that longitudinal optical phonons dominate the electron–phonon coupling and the coupling strength is much more robust in CsSnBr 3 than in CsSnI 3 . The PL intensity of CsSn X 3 microplates is suppressed due to the enhanced non-radiative relaxation and exciton dissociation competing with radiative recombination. According to the Arrhenius law, the exciton binding energy of CsSnBr 3 is ∼38.4 meV, slightly smaller than that of CsSnI 3 .
ISSN:1674-1056
2058-3834
DOI:10.1088/1674-1056/ad028e