Impacts of the Lattice Strain on Light Emission in Layered Perovskite Thin flakes

Author:

Zhang Zhonglong12,Zhou Runhui2,Li Meili2,Zhang Yan‐Fang3,Mo Yepei2,Yu Yang12,Xu Zhangsheng2,Sun Boning12,Wu Wenqiang24,Lu Qiuchun12,Lu Nan2,Xie Jin5,Mo Xiaoming1,Du Shixuan36,Pan Caofeng124ORCID

Affiliation:

1. Center on Nanoenergy Research, Institute of Science and Technology for Carbon Peak & Neutrality; Key Laboratory of Blue Energy and Systems Integration (Guangxi University), Education Department of Guangxi Zhuang Autonomous Region; School of Physical Science & Technology Guangxi University Nanning 530004 P. R. China

2. Beijing Institute of Nanoenergy and Nanosystems Chinese Academy of Sciences Beijing 101400 P. R. China

3. Institute of Physics & University of Chinese Academy of Sciences Chinese Academy of Sciences Beijing 100190 P. R. China

4. Institute of Atomic Manufacturing Beihang University Beijing 100191 P. R. China

5. State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano‐optoelectronics, School of Physics Peking University Beijing 100871 P. R. China

6. Songshan Lake Materials Laboratory Dongguan 523808 P. R. China

Abstract

AbstractStrain engineering, as a non‐chemical tuning knob, can enhance the performance of semiconductor devices. Here, an efficient manipulation of light emission is revealed in thin‐layered 2D perovskite strongly correlated to layer numbers of [PbI6]4− octahedron (n) and [C6H5(CH2)2NH3]2(CH3NH3)n‐1PbnI3n+1 (N) by applying uniaxial strains (ɛ) via bending the flexible substrate. As <n> increases from 1 to 3, an efficient light emission redshift (ɛ from −0.97% to 0.97%) is observed from bandgap shrinkage, and the shrinkage rate increases from 1.97 to 10.38 meV/%, which is attributed to the predominant uniaxial intralayer deformation due to the anisotropy of the [PbI6]4− octahedron lattice strain. Conversely, as <N> increases from 7 to 48 for n = 3, the deformation related to bandgap shrinkage rate is more prominent in small‐N flakes (<N> ≈ 7, 15.2 meV/%) but is easily offset in large‐N flakes (<N> ≈ 48, 7.7 meV/%). This anisotropic lattice deformation, meanwhile, inevitably modulates the carrier recombination dynamics of [C6H5(CH2)2NH3]2(CH3NH3)n‐1PbnI3n+1, which is essential for the development of highly efficient photoelectronic devices.

Funder

National Natural Science Foundation of China

Natural Science Foundation of Beijing Municipality

Fundamental Research Funds for the Central Universities

Publisher

Wiley

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