高性能量子点编码磁性微球的制备

基于改进的层层组装法,以氯仿/正丁醇混合溶液作为反应溶剂,将油溶性CdSSe/ZnS量子点装载到表面氨基修饰的磁性聚苯乙烯微球(MS)表面,通过调节量子点浓度,制备出高性能CdSSe/ZnS量子点编码磁性微球(CdSSe/ZnS-MBs).研究了氯仿和氯仿/正丁醇混合溶液对CdSSe/ZnS-MBs制备效果的影响.结果表明,氯仿/正丁醇混合溶液不仅能避免氯仿等量子点良溶剂对聚合物微球的形貌破坏,同时能促进CdSSe/ZnS量子点高效地装载到磁性微球表面.所制备的CdSSe/ZnS-MBs在水相具有较好的分散性,荧光强度变异系数(CV)小,形貌均一.该方法为简单、精确可控地制备高编码容量的量子点编码微球提供了新思路.     

Solid luminescent CdSe‐thiolated porous phosphate heterostructures. Application in fingermark detection in different surfaces

A fluorescent hybrid material (PPH‐S‐CdSe), which comprises cadmium selenide sulphide nanoparticles assembled onto thiol functionalised porous phosphate heterostructures (PPH‐SH), was synthesised in aqueous media. This material presents a high stability towards photo‐degradation. The obtained nanocomposite was characterised by various techniques such as Fourier transform infrared spectroscopy, energy dispersive X‐ray, transmission electron microscopy (TEM), X‐ray diffraction, X‐ray photoelectron spectroscopy and fluorescence spectroscopy. This fluorescent material showed a red emission at 576 nm combined with other at 473 nm, explained as different CdS_0.42Se_0.58 nanoparticles size, supported by TEM images. It was suitable for latent fingermark analysis in a wide range of surfaces. Because of its sensitivity and low cost, it is an actual alternative to conventional powdering materials. Copyright © 2012 John Wiley & Sons, Ltd.     

玻璃中CdSSe纳米晶体的光谱性能

对掺有镉、硒、硫的玻璃在650—800℃退火4?h，生长了不同尺寸的CdS0.13Se0.87纳米晶体，测量了纳米晶体的吸收光谱、光致发光（PL）谱和电调制光谱，确定了纳米晶体部分电子态的能量，讨论了CdSSe纳米晶体的光学性质与其尺寸之间的依赖关系.随着纳米晶体尺寸的增大，对应激子的吸收峰、PL峰及电吸收信号发生红移，表现出明显的量子尺寸效应.小尺寸纳米晶体的电吸收表现为量子受限的Stark效应，而大尺寸纳米晶体的电吸收线形与体材料的相似；随着纳米晶体尺寸的增大，电吸收信号增强.所有尺寸的纳米晶体都表现 关键词： CdSSe纳米晶体 吸收光谱 光致发光谱 电光响应     

Vibrational Raman spectra of CdSx Se1‐x magic‐size nanocrystals

Resonant Raman scattering spectra of ultrasmall (<2 nm) magic‐size nanocrystals (NCs) are reported. The spectra of CdS and CdS_x Se_1‐x NCs, resonantly excited with 325 nm and 442 nm laser lines, correspondingly, reveal broad features in the range of bulk optical phonons. The relatively large width, ～50 cm^‐1, and downward shift, ～20 cm^‐1, of the Raman bands with respect to the longitudinal optical phonon in bulk crystals and large NCs are discussed based on the breaking of the translational symmetry and bond distortion in these ultrasmall NCs. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)