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近单分散绝缘体 CsPbX(X = Cl、Br、I)纳米晶、它们的混合卤化物组成及其转化为 CsPbX 纳米晶。

Nearly Monodisperse Insulator CsPbX (X = Cl, Br, I) Nanocrystals, Their Mixed Halide Compositions, and Their Transformation into CsPbX Nanocrystals.

机构信息

Nanochemistry Department, Istituto Italiano di Tecnologia , Via Morego 30, 16163 Genova, Italy.

Dipartimento di Chimica e Chimica Industriale, Università degli Studi di Genova , Via Dodecaneso, 31, 16146, Genova, Italy.

出版信息

Nano Lett. 2017 Mar 8;17(3):1924-1930. doi: 10.1021/acs.nanolett.6b05262. Epub 2017 Feb 20.

Abstract

We have developed a colloidal synthesis of nearly monodisperse nanocrystals of pure CsPbX (X = Cl, Br, I) and their mixed halide compositions with sizes ranging from 9 to 37 nm. The optical absorption spectra of these nanocrystals display a sharp, high energy peak due to transitions between states localized in individual PbX octahedra. These spectral features are insensitive to the size of the particles and in agreement with the features of the corresponding bulk materials. Samples with mixed halide composition exhibit absorption bands that are intermediate in spectral position between those of the pure halide compounds. Furthermore, the absorption bands of intermediate compositions broaden due to the different possible combinations of halide coordination around the Pb ions. Both observations are supportive of the fact that the [PbX] octahedra are electronically decoupled in these systems. Because of the large band gap of CsPbX (>3.2 eV), no excitonic emission in the visible range was observed. The CsPbBr nanocrystals can be converted into green fluorescent CsPbBr nanocrystals by their reaction with an excess of PbBr with preservation of size and size distributions. The insertion of PbX into CsPbX provides a means of accessing CsPbX nanocrystals in a wide variety of sizes, shapes, and compositions, an important aspect for the development of precisely tuned perovskite nanocrystal inks.

摘要

我们开发了一种近单分散的纯 CsPbX(X = Cl、Br、I)纳米晶及其混合卤化物组成物的胶体合成方法,尺寸范围从 9 到 37nm。这些纳米晶的光学吸收光谱显示出一个由于 PbX 八面体中局域态之间跃迁而产生的尖锐、高能的峰。这些光谱特征对颗粒尺寸不敏感,与相应的体材料的特征一致。具有混合卤化物组成的样品表现出的吸收带位于纯卤化物化合物之间的光谱位置之间的中间位置。此外,由于 Pb 离子周围卤化物配位的不同可能组合,中间组成的吸收带变宽。这两个观察结果都支持这样一个事实,即在这些体系中,[PbX]八面体在电子上是解耦的。由于 CsPbX 的带隙较大(>3.2eV),在可见光范围内没有观察到激子发射。CsPbBr 纳米晶可以通过与过量的 PbBr 反应转化为绿色荧光 CsPbBr 纳米晶,同时保持尺寸和尺寸分布不变。PbX 的插入为 CsPbX 纳米晶提供了一种在各种尺寸、形状和组成的情况下获得 CsPbX 纳米晶的方法,这对于精确调谐钙钛矿纳米晶油墨的发展是一个重要方面。

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