Controlling and optimizing amplified spontaneous emission based on CsPbBr3@MCM-41 molecular sieve composite

材料科学 分子筛 放大自发辐射 复合数 激光阈值 聚合物 钙钛矿(结构) 筛子(范畴论) 热稳定性 涂层 旋涂 光电子学 激光器 复合材料 化学工程 化学 光学 数学 离散数学 有机化学 催化作用 物理 工程类 波长
作者
Zhaoping Chen,Aiqin Wang,Ziyao He,Jiaming Li,Enrou Mei,Xiaojuan Liang,Weidong Xiang
出处
期刊:Journal of Luminescence [Elsevier BV]
卷期号:253: 119411-119411
标识
DOI:10.1016/j.jlumin.2022.119411
摘要

CsPbX 3 (X = Cl, Br, I) perovskites have emerged as promising candidate lasing materials due to their high optical gain, low defect state density, and high absorption coefficient. Unfortunately, they suffer from poor stability, particularly with respect to temperature, moisture, and light exposure, preventing their use in practical optoelectronic applications, such as for amplified spontaneous emission (ASE) with an ultralow laser threshold. Herein, CsPbBr 3 @MCM-41 molecular sieve (CMM) composites are controllably prepared by different ultrasonication and stirring treatments. In addition, different perovskite concentrations and heat-treatment conditions are also considered to demonstrate the ASE behaviors. In addition, CMM@PS (CMMP) and CMM@AB (CMMA) composites were fabricated successfully by further optimizing the mixing ratio of CMM and the polymer. More excitingly, the stability of the CMM@polymer films with respect to the external environment is greatly improved after the polymer coating. To our surprise, the CMM@ploymer thin films demonstrated ASE at room-temperature, with an ASE threshold as low as 0.136 mJ/cm 2 and 0.049 mJ/cm 2 for CMMA and CMMP, respectively. These results clearly shed light upon the control and optimization of CsPbBr 3 perovskite composite films, paving the way for their widespread use in optoelectronic applications. • The composite films were prepared by one-step spin coating. • The as-prepared film can effectively avoid the instabilities to water and thermal. • SE of the films can be realized by optimizing the pretreatment conditions. • The threshold of ASE can be as low as 0.136 mJ/cm 2 .
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