壳层相关的CdSe核/壳量子点发光的热稳定性

测量了CdSe/ZnS(3 ML)核/壳结构及CdSe/CdS(3 ML)/ZnCdS(1 ML)/ZnS(2 ML)核/多壳层结构量子点在80~460 K范围内的光致发光光谱,研究了壳层结构对CdSe量子点发光热稳定性的影响。详细地分析了CdSe量子点的发光峰位能量、线宽和积分强度与温度之间的关系,发现CdSe量子点的发光热稳定性依赖于壳层结构。CdS/ZnCdS/ZnS多壳层结构包覆CdSe量子点在低温和高温部分的热激活能均大于ZnS壳层包覆的CdSe量子点,具有更好的发光热稳定性。此外,在300-460-300 K加热-冷却循环实验中,CdS/ZnCdS/ZnS多壳层结构包覆CdSe量子点的发光强度永久性损失更少,热抵御能力更强。     

CdSe/CdS核壳量子点复合材料合成及其在白光发光二极管中的应用

采用有机化学合成法,利用正三辛基膦(TOP)辅助的快速注入生长方法,改进传统的制备工艺,实现了CdSe/CdS厚壳层核壳(8.6 ML)量子点复合材料的合成制备,并对所合成的核、核壳量子点及其复合材料的晶格结构、形貌特点与发光性质进行了XRD、TEM、SEM、UV-Vis、PL表征和红光补偿效果测试。测试结果表明,CdSe核具有立方纤锌矿晶格结构;CdSe/CdS量子点复合材料直径为45~75μm,呈菱形规则形貌,且颗粒分散性良好。采用该方法,可以提高量子产率,产率由4%(CdSe核)升至48%(CdSe/CdS核壳量子点);可以增强激子态发光能力,CdSe/CdS核壳量子点复合材料的荧光强度约为CdSe核的13倍。将该材料与YAG∶Ce~(3+)黄色荧光粉组合应用,获得了高光效(148.29 lm/W)、高显色指数(Ra为90.1,R9为97.0)的白光发光二级管,表明按照上述方法获得的CdSe/CdS核壳量子点复合材料在白光发光二极管中深红光波段具有较好的补偿效果。     

单核/双壳结构CdSe/CdS/ZnS纳米晶的合成与发光性质

以巯基乙酸为稳定剂,在水溶液中合成了单核/双壳结构的CdSe/CdS/ZnS纳米晶。在内核CdSe和外壳ZnS之间的内壳CdS作为晶格匹配调节层,能够很好的改善核/壳界面处的性能,而且,最外层ZnS能够最大程度地使激子受限。用TEM和XPS对纳米晶进行了表征,并且用光致发光光谱和吸收光谱对不同核壳结构的纳米晶的发光性能进行了比较,结果表明单核/双壳结构的纳米晶具有更加优异的发光特性。     

CdTe/CdS核壳结构量子点超快载流子动力学

在水相合成CdTe以及CdTe/CdS核壳结构量子点基础上, 利用基于抽运-探测技术的瞬态差分透射技术研究了CdTe量子点以及不同CdS壳层厚度的CdTe/CdS量子点的最低激子能态的超快激发与弛豫动力学. 研究表明:相比于CdTe,CdTe/CdS量子点的电子空穴由于空间分离,其所需的激发时间要长于电子空穴空间重叠态所需要的激发时间.随着壳层厚度的增加, 量子点表面的钝化有效地减少了表面态相关弛豫机理,并延长相对应的弛豫时间.     

CdSe/CdS核壳纳米晶微波水热法一步合成与发光光谱分析

采用微波水热法一步合成了核壳结构的CdSe/CdS纳米晶,讨论了巯基丙酸中S^2-的释放过程对纳米晶生长的影响。XRD和Raman光谱结果表明,140℃合成温度下获得了CdSe/CdS核壳结构的纳米晶。FTIR光谱结果表明,巯基丙酸随时间的分解有助于CdS壳层的形成。PL光谱呈现出CdSe纳米晶的带间发射和缺陷发射,随着核壳结构的形成,CdSe纳米晶的表面缺陷被抑制,相关的荧光发射减弱。     

核壳结构硒化镉/硫化镉/巯基乙酸量子点载流子输运特性

采用水溶液法合成了巯基乙酸(TGA) 包覆的CdSe 量子点. 通过X 射线粉末衍射和高分辨透射显微镜检测结果证实, 合成得到闪锌矿结构CdSe 量子点. 能谱图和傅里叶变换红外光谱图结果说明, 在核CdSe 纳米粒子表面与配体TGA 之间有CdS 壳层结构形成. 利用样品表面光电压(SPV) 谱, 指认CdSe 量子点精细能带结构以及各自对应的激发态特征: 475 nm (2.61 eV) 和400 nm (3.1 eV) 两个波长处的SPV 响应峰分别与CdSe 核和CdS 壳层带-带隙跃迁相对应; 370 nm (3.35 eV) 附近SPV 响应峰可能与TGA 中羰基与巯基或羧基之间发生的n →π^* 跃迁有关. 场诱导表面光电压谱结果证实, 合成的CdSe 量子点具有明显的N 型表面光伏特性, 而上述n→π^* 跃迁则具有P 型表面光伏特性. 荧光光谱谱线均匀增宽以及SPV 响应峰位蓝移, 说明样品具有明显的量子尺寸效应. 结合不同pH 值下合成的CdSe 量子点的SPV 谱和表面光声谱发现, SPV 响应强度与表面光声光谱信号强度变化趋势恰好相反. 上述样品表面光伏效应表明, CdSe 量子点表面和相界面处的精细电子结构以及光生载流子的输运特性均与量子点的尺寸大小存在某种内在联系. 关键词： 硒化镉量子点 光生载流子 表面光电压谱 表面光声光谱     

CdSe/ZnSe/ZnS多壳层结构量子点的制备与表征

展示了一种简捷的多壳层量子点合成路线。在含有过量Se源的CdSe体系中直接注入Zn源,"一步法"合成了CdSe/ZnSe量子点;进一步以CdSe/ZnSe为"核",表面外延生长ZnS壳层制备了核/壳/壳结构CdSe/ZnSe/ZnS量子点。相对于以往报道的多壳层结构量子点的制备方法,该方法通过减少壳层的生长步骤有效地简化了实验操作,缩短了实验周期,同时减少对原料的损耗。对量子点进行高温退火处理,能够大幅提高CdSe/ZnSe/ZnS量子点的发光量子产率。透射电镜、XRD以及光谱研究表明:所制备的量子点接近球形,核与壳层纳米晶均为闪锌矿结构,最终获得的CdSe/ZnSe/ZnS量子点的光致发光量子产率达到53％。为了实现量子点的表面生物功能化,通过巯基酸进行了表面配体交换修饰,使量子点表面具有水溶性的羧基功能团,并且能够维持较高的光致发光量子产率。     

谷胱甘肽包被的CdSe/CdS量子点的直接水相制备及其对人血淋巴细胞的标记成像

首次用谷胱甘肽(GSH)作为稳定剂,在水溶液中制备了稳定地发射绿色荧光和橙色荧光的两种 CdSe/CdS核/壳结构的纳米量子点。用紫外-可见分光光度和荧光光谱方法研究了CdSe/CdS量子点的发光特性。透射电镜(TEM)结果表明CdSe/CdS量子点近似球形,在水中分散性良好,比CdSe量子点具有更优异的发光特性,发射光谱和吸收光谱都有红移现象。将CdSe/CdS量子点与鼠抗人CD3抗体连接,制备了水溶性CdSe/CdS-CD3复合物探针,对人血淋巴细胞进行标记和成像。结果表明用该探针对人血淋巴细胞成像清晰,其荧光在30 min的连续蓝光激发下无明显衰退,而FITC荧光在20 min内基本完全猝灭。     

AlGaAs/GaAs多量子阱结构中受激载流子的飞秒弛豫特性

本文介绍采用飞秒饱和吸收测量技术研究Al_xGa_(1-x)As/GaAs多量子阱结构中受激载流子的超快弛豫特性.当激发光子能量大于样品势垒层能带隙时,受激产生于势垒层和势阱层连续态中的载流子分别在130和30fs时间内离开受激态,弛豫至准平衡态.势垒中的载流子被捕至势阱束缚态的情况主要发生于热载流子的冷却和复合过程的皮秒级时间内.     

HgTe/CdS/ZnS多壳层量子点的制备与表征

采用一种简单的方法合成HgTe/CdS/ZnS多壳层量子点。首先,以1-硫代甘油为稳定剂,在水相溶液中制备出HgTe核量子点;然后,采用外延生长法依次在HgTe核量子点表面包覆CdS和ZnS壳层,合成出最终具有稳定近红外发光的HgTe/CdS/ZnS多壳层量子点。该合成方法仅需3个步骤,具有操作简单、成本低廉的优点。实验结果显示,当反应温度为90 ℃、反应溶液pH为11.0、反应加热回流时间为4 min时,HgTe/CdS/ZnS多壳层量子点具有最高荧光量子产率36%。     

Ultrafast spectroscopy of CdS/CdSe quantum dots

Results from the nonresonance spectroscopy of CdS/CdSe quantum dots (composites of CdSe–CdS nanoparticles (core–shell)) are presented. The nonlinear optical properties of CdS/CdSe QDs in PMMA are studied with fs pulses at 1053 nm using the transient lens technique. QDs generate rapidly oscillating signals with amplitude rise times of around 200 fs and decay times of around 500 fs, while pure PMMA polymer only generates an oscillating signal whose envelope coincides with its autocorrelation function.     

CdSe/CdS核/壳型纳米晶的光谱特性

以巯基乙酸为稳定剂制备了CdSe/CdS核／壳型纳米晶。用光吸收谱（Abs)、光致发光谱（PL）及光致发光激发谱（PLE）研究了CdS壳层对CdSe纳米晶电子结构，从而对其吸收和发光性能的影响。根据PL和PLE的结果以及带边激子精细结构的计算结果，我们用尺寸很小的纳米晶中所形成的基激缔合物解释了PL光谱与吸收边之间较大的Stokes位移。     

Wurtzite and zinc-blende CdSe based core/shell semiconductor nanocrystals: Structure, morphology and photoluminescence

We report comparative study of core/shell nanocrystals based on wurtzite and novel zinc-blende CdSe core. Both wurtzite and zinc-blende CdSe are coated with CdS shell or CdS/ZnS multishell under identical synthetic parameters. Crystal structure analysis finds that CdS shell is wurtzite on either wurtzite or zinc-blende CdSe cores. Morphology and photoluminescence studies exhibit that for zinc-blende CdSe based samples, the shell growth is in fine epitaxy and the obtained core/shell nanocrystals show high quantum yield both before and after surface modification process; while wurtzite CdSe based samples have irregular shape indicating inhomogeneous shell growth, and are with lower quantum yield. Furthermore, in the photoluminescence spectra exited with UV radiation, wurtzite CdSe based samples show side peaks of independently nucleated nanocrystals from the shell material; while samples with zinc-blende CdSe cores are potent in restricting these byproducts, which may attribute to the highly effective arrestment of precursor ions onto the zinc-blende CdSe surface. These features manifest that zinc-blende CdSe is more talented than conventional wurtzite CdSe in achieving core/shell nanocrystals with higher qualities.     

Atomistic tight-binding computations of the structural and optical properties of CdTe/CdX (X=S and Se)/ZnS core/shell/shell nanocrystals

A study of CdTe/CdX (X=S and Se)/ZnS core/shell/shell nanocrystals is carried out using atomistic tight-binding theory and the configuration interaction method to provide information for applications in bioimaging, biolabeling, display devices and near-infrared electronic instruments. The calculations yield the dependences of the internal and external passivated shells on the natural behaviours of CdTe/CdX (X=S and Se)/ZnS core/shell/shell nanocrystals. The reduction of the optical band gaps is observed with increasing numbers of monolayers in the external ZnS shell due to quantum confinement. Interestingly, the optical band gaps of CdTe/CdS/ZnS core/shell/shell nanocrystals are greater than those of CdTe/CdSe/ZnS core/shell/shell nanocrystals. In the presence of an external ZnS-coated shell, electron–hole wave function overlaps, oscillation strengths, ground-state exchange energies and Stokes shift are improved, whereas ground-state coulomb energies and fine-structure splitting are reduced. The oscillation strengths, Stokes shift and fine-structure splitting are reduced with the increase in external ZnS shell thickness. The oscillation strengths, Stokes shift and fine-structure splitting of CdTe/CdS/ZnS core/shell/shell nanocrystals are larger than those of CdTe/CdSe/ZnS core/shell/shell nanocrystals. Reduction of the atomistic electron–hole interactions is observed with increasing external ZnS shell size. The strong electron–hole interactions are more probed in CdTe/CdS/ZnS core/shell/shell nanocrystals than in CdTe/CdSe/ZnS core/shell/shell nanocrystals.     

A novel two-phase thermal approach for synthesizing CdSe/CdS core/shell nanostructure

CdSe/CdS core/shell nanocrystals have been synthesized through a low cost and simple two-phase thermal route. The optical spectroscopy and structural characterization evidenced the core/shell structure of the CdSe/CdS nanoparticles. The X-ray diffraction patterns of CdSe and CdSe/CdS nanoparticles exhibited peak positions corresponding to those of their bulk cubic crystal structures. The X-ray photoelectron spectroscopy data confirmed the elemental composition of the CdSe/CdS nanoparticles. The absorption spectra of core/shell nanoparticles showed red shift with respect to the core CdSe nanoparticles. The photoluminescence study indicates that the intensity of the emission maximum is considerably increased in the core/shell structure as compared with the parent material, and the capping of CdS nanoparticles with CdSe material exhibit a near band-edge emission, indicating a successful passivation by removing surface defects. The high-resolution transmission microscope images of the bare and core/shell nanoparticles ascertained the monodispersed and well-defined spherical particles. The average particle sizes for CdSe and CdSe/CdS nanoparticles are 2.5 and 5 nm, respectively, thus confirming, the larger diameter of CdSe/CdS core/shell nanostructure than the core CdSe nanoparticles.     

Evolution of Luminescence with Shell's Thickness in Colloidal CdSe/CdS Core/Shell Quantum Dots

We synthesize colloidal CdSe/CdS core/shell quantum dots with different shell thicknesses, and there are five samples including CdSe core dots, and CdSe/CdS core/shell dots with 1-4 CdS layers. X-ray diffraction and Raman measurements indicate that the stress in CdSe core becomes stronger with the increasing shell thickness, and the optical measurements show that when the shell becomes thicker, the photoluminescence quantum yield is enhanced, and the radiative decay is also expedited. The temperature-dependent optical spectra are measured. The relation between the microstructure and the optical properties is discussed.     

Evidence of electron wave function delocalization in CdSe/CdS asymmetric nanocrystals

We studied the delocalization of electron wave function in asymmetric CdSe/CdS nanocrystals, consisting of a spherical CdSe dot embedded in an elongated CdS shell, by means of a pump–probe technique. By comparing the transient spectra obtained upon pumping the band edge transition of the CdSe in CdSe/CdS heterostructure and in a bare CdSe dot, we observed the delocalization of electron wave function at the CdSe/CdS interface.