Stereo‐Hindrance Engineering of A Cation toward <110>‐Oriented 2D Perovskite with Minimized Tilting and High‐Performance X‐Ray Detection

Author:

Xia Mengling1ORCID,Sun Xijuan1,Ye Fan2,Liao Mingquan1,Liu Jiaqi1,Liu Shiyou2,Wu Dong1,Xu Yinsheng1,Zhang Xianghua13,Xue Kan‐Hao24,Miao Xiangshui4,Tang Jiang2,Niu Guangda2ORCID

Affiliation:

1. School of Materials Science and Engineering and State Key Laboratory of Silicate Materials for Architectures Wuhan University of Technology Wuhan 430070 China

2. Wuhan National Laboratory for Optoelectronics (WNLO) Huazhong University of Science and Technology (HUST) Wuhan 430074 China

3. Laboratoire des Verres et Céramiques UMR‐CNRS 6226 Sciences chimiques de Rennes Université de Rennes 1 Rennes 35042 France

4. School of Integrated Circuits Huazhong University of Science and Technology (HUST) Wuhan 430074 China

Abstract

Abstract2D <100>‐oriented Dion–Jacobson or Ruddlesden–Popper perovskites are widely recognized as promising candidates for optoelectronic applications. However, the large interlayer spacing significantly hinders the carrier transport. <110>‐oriented 2D perovskites naturally exhibit reduced interlayer spacings, but the tilting of metal halide octahedra is typically serious and leads to poor charge transport. Herein, a <110>‐oriented 2D perovskite EPZPbBr4 (EPZ = 1‐ethylpiperazine) with minimized tilting is designed through A‐site stereo‐hindrance engineering. The piperazine functional group enters the space enclosed by the three [PbBr6]4− octahedra, pushing Pb─Br─Pb closer to a straight line (maximum Pb─Br─Pb angle ≈180°), suppressing the tilting as well as electron–phonon coupling. Meanwhile, the ethyl group is located between layers and contributes an extremely reduced effective interlayer distance (2.22 Å), further facilitating the carrier transport. As a result, EPZPbBr4 simultaneously demonstrates high µτ product (1.8 × 10−3 cm2 V−1) and large resistivity (2.17 × 1010 Ω cm). The assembled X‐ray detector achieves low dark current of 1.02 × 10−10 A cm−2 and high sensitivity of 1240 µC Gy−1 cm−2 under the same bias voltage. The realized specific detectivity (ratio of sensitivity to noise current density, 1.23 × 108 µC Gy−1 cm−1 A−1/2) is the highest among all reported perovskite X‐ray detectors.

Funder

National Natural Science Foundation of China

Publisher

Wiley

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