3D/2D Core-Shell CsPbBr₃ Microcrystals for Stable X-Ray Detection and Imaging

Although metal halide perovskite (MHP) materials are promising candidates for direct X-ray detection, the surface and internal defects of perovskite polycrystalline thick films lead to severe noise current and poor device stability. Herein, a phenylethylammonium (PEA+) cladding layer was integrated with 3D CsPbBr3 grains, forming 3D/2D core-shell CsPbBr3 perovskite microcrystals. The PEA+, acting as the A-site cation, is able to passivate the surface defects, while the forming 2D perovskite cladding layer inhibits ion migration within CsPbBr3 grains. The blade-coated polycrystalline 3D/2D core-shell CsPbBr3 perovskite thick film exhibits a reduced trap density from <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${4}.{32}\times {10} ^{{10}}$ </tex-math></inline-formula> cm−3 to <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${4}.{26}\times {10} ^{{9}}$ </tex-math></inline-formula> cm−3 compared to conventional CsPbBr3 film, with ion migration activation energy increasing from 123 meV to 210 meV. Consequently, the obtained perovskite X-ray detector exhibits a high sensitivity of 29,<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$460~\mu $ </tex-math></inline-formula> C Gy<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${}_{\text {air}}^{-{1}}$ </tex-math></inline-formula> cm−2 and a low detection limit of 84 nGyair s−1 (50 keV X-ray photon energy), and the detector maintains long-term operational stability with a dark current drift as low as <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${4}.{12}\times {10} ^{-{5}}$ </tex-math></inline-formula> nA mm−1 s−1 V−1. Furthermore, we integrated the 3D/2D core-shell polycrystalline CsPbBr3 with a TFT chip (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${64}\times {64}$ </tex-math></inline-formula> array) and successfully obtained a clear and high-contrast X-ray image of a mouse’s paw exhibiting a spatial resolution of 2.5 lp mm−1.

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Publication Details

Journal
IEEE Electron Device Letters
Published
2025-04-01
DOI
https://doi.org/10.1109/led.2025.3556477
Citations
2
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
1.46

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article

3D/2D Core-Shell CsPbBr₃ Microcrystals for Stable X-Ray Detection and Imaging

Bin Tian, Xue‐Feng Yu, Wenjie Luo, Xingchen He et al.
2 citations
IEEE Electron Device Letters
Perovskite Materials and Applications
1.46
article

3D/2D Core-Shell CsPbBr₃ Microcrystals for Stable X-Ray Detection and Imaging

Bin Tian, Xue‐Feng Yu, Wenjie Luo, Xingchen He, Zhiyuan Liu, Yang Zhang, Xiaoli Wang, Dong Li, Yanliang Liu, Boyoung Han, Xingzhou Su, Wenxuan Yang
article en
2 citations

Abstract

Although metal halide perovskite (MHP) materials are promising candidates for direct X-ray detection, the surface and internal defects of perovskite polycrystalline thick films lead to severe noise current and poor device stability. Herein, a phenylethylammonium (PEA+) cladding layer was integrated with 3D CsPbBr3 grains, forming 3D/2D core-shell CsPbBr3 perovskite microcrystals. The PEA+, acting as the A-site cation, is able to passivate the surface defects, while the forming 2D perovskite cladding layer inhibits ion migration within CsPbBr3 grains. The blade-coated polycrystalline 3D/2D core-shell CsPbBr3 perovskite thick film exhibits a reduced trap density from <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${4}.{32}\times {10} ^{{10}}$ </tex-math></inline-formula> cm−3 to <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${4}.{26}\times {10} ^{{9}}$ </tex-math></inline-formula> cm−3 compared to conventional CsPbBr3 film, with ion migration activation energy increasing from 123 meV to 210 meV. Consequently, the obtained perovskite X-ray detector exhibits a high sensitivity of 29,<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$460~\mu $ </tex-math></inline-formula> C Gy<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${}_{\text {air}}^{-{1}}$ </tex-math></inline-formula> cm−2 and a low detection limit of 84 nGyair s−1 (50 keV X-ray photon energy), and the detector maintains long-term operational stability with a dark current drift as low as <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${4}.{12}\times {10} ^{-{5}}$ </tex-math></inline-formula> nA mm−1 s−1 V−1. Furthermore, we integrated the 3D/2D core-shell polycrystalline CsPbBr3 with a TFT chip (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${64}\times {64}$ </tex-math></inline-formula> array) and successfully obtained a clear and high-contrast X-ray image of a mouse’s paw exhibiting a spatial resolution of 2.5 lp mm−1.

IEEE Electron Device LettersVol. 46(6)
Shenzhen Institutes of Advanced Technology (CN), University of Chinese Academy of Sciences (CN)
National Natural Science Foundation of China, Basic and Applied Basic Research Foundation of Guangdong Province
Openalex Percentile: Top 18%
Perovskite Materials and Applications
1.46
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