可控结构非晶化使零维(C6H5CH2NH3)3InBr6可调谐发射

IF 13.7 Q1 CHEMISTRY, MULTIDISCIPLINARY
Qian Li, Bin Xu, Xiaofan Xu, Yayun Wang, Zewei Quan
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引用次数: 0

摘要

零维(0D)杂化金属卤化物(HMHs)作为多功能发射体具有很大的前景。然而,有机部分的精确功能化和无机多面体自捕获激子(STE)发射的可控调制仍然是一个挑战。本研究引入0D (PMA)3InBr6 (PMA+ = C6H5CH2NH3+)作为多功能发射器,利用压力诱导的结构调节来控制光致发光特性。压力的增加导致InBr63−八面体同时收缩和扭曲,STE的发射颜色从橙色变为绿色。在高压缩时,结构非晶化会抑制STE的发射,但在压力释放后,PMA+阳离子会发出明亮的青色发射,其强度约为初始STE发射的21倍。增强的发射归因于分子构型的改变,分子间接触的破坏和晶格振动的减少,共同抑制了准分子耦合并最小化了恢复的非晶相的非辐射损失。此外,通过激光诱导的结构非晶化也实现了发射转换,扩大了(PMA)3InBr6在直接激光写入和敏感激光探测应用方面的潜力。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Tunable Emissions in Zero-Dimensional (C6H5CH2NH3)3InBr6 Enabled by Controlled Structural Amorphization

Tunable Emissions in Zero-Dimensional (C6H5CH2NH3)3InBr6 Enabled by Controlled Structural Amorphization

Zero-dimensional (0D) hybrid metal halides (HMHs) hold great promise as multifunctional emitters. However, precise functionalization of organic moieties and controlled modulation of self-trapped exciton (STE) emission from inorganic polyhedra remain challenging. This study introduces 0D (PMA)3InBr6 (PMA+ = C6H5CH2NH3+) as a multifunctional emitter, leveraging pressure-induced structural regulation to control photoluminescence properties. Increasing pressure leads to simultaneous contraction and distortion of InBr63− octahedra, shifting the STE emission color from orange to green. At high compression, structural amorphization quenches STE emission, but upon pressure release, a bright cyan emission from the PMA+ cation emerges, with intensity approximately 21 times stronger than that of the initial STE emission. The enhanced emission is attributed to altered molecular configurations, disrupted intermolecular contacts, and reduced lattice vibrations, collectively suppressing excimeric coupling and minimizing nonradiative losses in the recovered amorphous phase. Furthermore, emission conversion is also achieved via laser-induced structural amorphization, expanding the potential of (PMA)3InBr6 for direct laser writing and sensitive laser detection applications.

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来源期刊
CiteScore
17.40
自引率
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