CdS/ZnO纳米复合结构制备及荧光特性研究

为增强CdS纳米粒子的荧光强度,以及稳定性,研究了Cd,S不同质量比,有无稳定剂等条件下CdS纳米粒子的制备及荧光特性。在碱性条件下,利用水热法合成了CdS/ZnO的纳米复合结构,并对所有样品进行了XRD、荧光光谱和SEM表征。测试结果表明所制备的CdS纳米粒子和CdS/ZnO的纳米复合结构粒子成分单一且纯净;ZnO复合在CdS表面;在紫外光(328.5 nm)激发下,CdS/ZnO纳米复合结构的发射峰位于463 nm处,峰形窄而对称,CdS/ZnO纳米复合结构的荧光强度比CdS纳米粒子的荧光强度有显著增强,且CdS和ZnO物质量之比为1∶1条件下,荧光强度最高,其荧光效率比单一CdS纳米粒子高出11%。通过第一性原理计算结果表明,CdS能带结构中,Cd-4d,S-3p和Cd-5s能带分别由5条、3条和1条能级构成,对比不同轨道的分态密度强度,看出CdS的导带边主要由Cd-5s轨道贡献,而价带边主要由S-3p轨道贡献,能量在-7 eV附近的电子态主要由Cd-4d轨道贡献。而ZnO上价带主要由O-2p电子构成,靠近费米能级的价带区域则主要由Zn-3d电子贡献,在导带部分,主要来源于Zn-4s和O-2p电子。由于在两种材料的复合结构中Zn-3d电子的能级和S-3p电子的能级接近,存在着二型带阶结构使能带变窄,容易形成跃迁,减小电子-空穴的复合,从而促进复合结构荧光效率的提高。     

镉掺杂氧化锌纳米花的制备及其光催化活性

以氯化锌、氯化镉、氢氧化钠为原料,采用水热法合成Cd掺杂纳米花状ZnO光催化剂,并通过该样品对罗丹明B水溶液的降解来研究其光催化活性。利用X射线衍射(XRD)、扫描电子显微镜(SEM)、X射线能量色散谱(EDS)、光致发光谱(PL)及紫外-可见分光光度计(UV-Vis)等测试手段对材料物性进行表征。实验结果表明:当掺杂Cd2+时,样品形貌发生变化、粒径减小;掺杂Cd2+后的ZnO的吸收边和紫外峰对比于纯ZnO均发生红移,禁带宽度由3.24 eV减小到3.16 eV。通过光催化实验分析可知,掺杂后纳米ZnO光催化剂对罗丹明B水溶液的降解率有所提高,光照3 h其降解率高达98%,说明与纯ZnO相比,Cd掺杂ZnO纳米花具有更高的光催化活性。     

镉掺杂氧化锌纳米花的制备及其光催化活性

以氯化锌、氯化镉、氢氧化钠为原料,采用水热法合成Cd掺杂纳米花状ZnO光催化剂,并通过该样品对罗丹明B水溶液的降解来研究其光催化活性。利用X射线衍射（XRD）、扫描电子显微镜（SEM）、X射线能量色散谱（EDS）、光致发光谱（PL）及紫外-可见分光光度计（UV-Vis）等测试手段对材料物性进行表征。实验结果表明：当掺杂Cd²⁺时,样品形貌发生变化、粒径减小;掺杂Cd²⁺后的ZnO的吸收边和紫外峰对比于纯ZnO均发生红移,禁带宽度由3.24 eV 减小到3.16 eV。通过光催化实验分析可知,掺杂后纳米ZnO光催化剂对罗丹明B 水溶液的降解率有所提高,光照3 h其降解率高达98%,说明与纯ZnO相比,Cd掺杂ZnO纳米花具有更高的光催化活性。     

溶胶-凝胶法制备纳米氧化锌及其光催化性能

采用溶胶-凝胶法制备ZnO纳米粒子,采用X-射线衍射仪(XRD)、透射电镜(TEM)等手段对样品进行了表征;以纳米氧化锌作为光催化剂,利用300W高压汞灯为光源对甲基橙溶液进行光催化实验。实验结果表明:以汞灯为光源,纳米ZnO为催化剂对甲基橙溶液进行光催化时,纳米ZnO的最佳投加量为0.1020g。     

纳米微晶结构ZnO及其紫外激光

本介绍了的年来研制Ⅱ-Ⅵ族半导体激光器的一个新的途径——ZnO的纳米微晶结构。它分为两大类别：即六角柱形蜂巢状结构和粉末状颗粒结构。都已在近紫外波段实现了室温下光泵激发的受激发射,它将是继Ⅱ-Ⅵ族硒化物和Ⅲ-Ⅳ氮化物之后的新型半导体激光器材料。     

纳米结构ZnO薄膜的制备及其疏水特性

利用水热法制备出与透明导电衬底附着良好的多种纳米结构ZnO薄膜,包括纳米柱阵列、纳米管阵列、纳米片阵列等,方便集成在多种器件上。并且实现了阵列中纳米柱、纳米管外径的调节,柱外径在50~300 nm范围内可调,管外径在300~1 000 nm范围内可调。几种纳米薄膜均显示出较强的疏水性。在未经任何低表面能物质修饰的情况下,水在外径约300 nm的管状阵列表面的静态接触角已达138°。而在紫外光照射下,这些疏水的ZnO薄膜还可以变得亲水。这些研究结果为ZnO纳米阵列在相关方面的应用提供了重要依据。     

强悬浮性纳米TiO2的制备、表征及光催化活性研究Ⅱ.光催化活性研究

将甲基橙溶液作为模拟废水,在紫外灯照射下,通过测量甲基橙溶液在470nm处吸光度的变化,考察了热分解制备纳米TiO2后处理过程中采用硅油淬火改性和自然冷却所得产物的光催化活性,并初步分析了两者光催化甲基橙的机理和在35min内的降解率和动力学反应过程。结果表明：两者均具有良好的光催化降解效果,且活性差别不大。但经硅油淬火改性的纳米TiO2因在水中具有强悬浮性,可更为有效地利用外部光源在工业废水的表层降解有害成分。     

铁镧复合氧化物纳米微粒的制备及其光催化性能

以溶胶-凝胶法制备了纳米铁镧复合氧化物。通过了XRD、TG-DTA等手段,对该氧化物进行了分析。研究了焙烧温度、光催化剂的用量、光照等因素对催化剂光催化降解活性染料的影响。并用红外光谱分析方法验证光催化降解效果。结果表明在适当的用量和700℃焙烧并在紫外光照射下铁镧复合氧化物对活性翠蓝KGL和活性B-GFF黑有较强的光催化降解活性。     

强悬浮性纳米TiO2的制备、表征及光催化活性研究(Ⅱ)光催化活性研究

将甲基橙溶液作为模拟废水,考察了热分解制备纳米TiO2后处理过程中采用硅油淬火改性和自然冷却所得产物的光催化活性。结果表明：两者均具有良好的光催化降解效果,且活性差别不大。但经硅油淬火改性的纳米TiO2因在水中具有强悬浮性,可更为有效地利用外部光源在工业废水的表层降解有害成分。     

TiO2花状纳米结构的制备及光催化性能

用Ti片和H2O2在较低的温度下通过控制反应时间制备了不同形貌的纳米TiO2.在80℃下反应10 min得到了和Ti片黏附较好的多孔纳米结构,延长反应时间先后得到了类花状和类棒状纳米结构．在80℃下反应4 h得到的纳米结构样品为非晶态,而反应10 h制备出以锐钛矿相为主的结晶态纳米结构．通过300℃退火得到的几乎是纯锐钛矿相的纳米TiO2．用紫外光照射降解RhB溶液的方法研究了纳米TiO2的光催化性能．结果表明7 cm2的退火后的类花状纳米TiO2降解染料分子的光催化效率是仅用紫外光降解的29．8倍．     

CdS/PbS co-sensitized ZnO nanorods and its photovoltaic properties

Nanoparticles co-sensitized nanorods were designed and prepared by assembled CdS and PbS nanoparticles over ZnO nanorods using successive ionic layer adsorption and reaction (SILAR) method. The results showed that the uniform CdS and PdS nanoparticles could be deposited on the lateral and top of the ZnO nanorods when the precursor concentration was 0.05 M and 0.02 M, respectively. Solar cells based on CdS and PbS nanoparticles sensitized ZnO nanorods arrays were assembled successfully. A cell efficiency of 0.38% was obtained in ZnO/CdS/PbS in comparison with ZnO/PbS/CdS mainly due to the stepwise band edge structure constructed in this system except the coverage density of nanoparticles.     

CdS/聚苯乙烯-丙烯基硫脲纳米复合材料的合成及表征

以二硫化碳、氯化镉和聚苯乙烯-丙烯胺为原料,用液相原位沉淀法合成CdS/聚苯乙烯-丙烯基硫脲纳米复合材料。产物通过X射线衍射、扫描电子显微镜、红外光谱、紫外-可见吸收光谱、荧光光谱进行了表征。     

Triple‐Yolked ZnO/CdS Hollow Spheres for Semiconductor‐Sensitized Solar Cells

A new kind of complex hollow structure, ZnO/CdS triple‐yolked hollow spheres (TYs), is prepared using a facile method. The formation mechanism is described in terms of a combined effect of the bubble‐assisted Ostwald ripening and appropriate ion‐exchange processes. The structural effect of ZnO hollow microspheres on the energy conversion efficiency is investigated. The uniqueness of TYs morphology leads to a 37% enhancement in energy conversion efficiency for SSSCs, as compared with single‐shelled hollow spheres. The method using controlled ZnO/CdS yolk‐in‐shell structures in SSSCs presents obvious advantages in the generation of light scattering and makes full use of the internal structures of the photoelectrode. It also provides a feasible synthetic approach for fabrication of other complex hollow structures made of multicomponent functional heteromaterials.     

High-quality CdS quantum dots sensitized ZnO nanotube array films for superior photoelectrochemical performance

The surface characteristics of ZnO were synthetically optimized by a self-designed simultaneous etching and W-doping hydrothermal method utilizing as-prepared ZnO nanorod (NR) array films as the template. Benefiting from the etching and regrowth process and the different structural stabilities of the various faces of ZnO NRs, the uniquely etched and W-doped ZnO (EWZ) nanotube (NT) array films with larger surface area, more active sites and better energy band structure were used to improve the photoelectrochemical (PEC) performance and the loading quality of CdS quantum dots (QDs). On the basis of their better surface characteristics, the CdS QDs were uniformly loaded on EWZ NT array film with a good coverage ratio and interface connection; this effectively improved the light-harvesting ability, charge transportation and separation as well as charge injection efficiency during the PEC reaction. Therefore, all the CdS QD-sensitized EWZ NT array films exhibited significantly enhanced PEC performance. The CdS/EWZ-7 composite films exhibited the optimal photocurrent density with a value of 12 mA· cm^-2, 2.5 times higher than that of conventional CdS/ZnO-7 composite films under the same sensitization times with CdS QDs. The corresponding etching and optimizing mechanisms were also discussed.     

CdS/膨润土复合材料的制备及其光催化性能

以CdCl₂和硫代乙酰胺为反应物,通过湿化学法合成CdS/膨润土复合材料,采用X射线衍射(XRD)、红外光谱(FTIR)以及紫外可见光谱(UV-Vis)等分析技术对其结构及光学性能进行表征。以罗丹明B和亚甲基蓝为目标污染物,考察了CdS/膨润土复合材料对有机染料的降解性能。结果表明:在罗丹明B和亚甲基蓝的初始浓度为20 mg/L 时,光照3 h后,CdS/膨润土对它们的降解率分别为80.6%和88.3%,优于CdS及膨润土原土催化剂。     

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%。     

核/壳结构ZnS : Mn/CdS纳米粒子的制备及发光

利用溶剂热法制备了Mn离子掺杂的ZnS纳米粒子(ZnS : Mn),利用沉淀法对ZnS ∶ Mn纳米粒子进行了不同厚度的CdS无机壳层包覆。采用X射线衍射(XRD)、透射电子显微镜(TEM)、X射线光电子能谱(XPS)及光致发光(PL)光谱等手段对样品进行了表征。TEM显示粒子为球形,直径大约在14~18 nm之间。由XRD结果可以看出CdS壳层的形成过程受到了ZnS ∶ Mn核的影响,导致其结晶较差。XRD和XPS测量证明了ZnS : Mn/CdS的核壳结构。随着CdS壳层的增厚,样品的发光强度呈现一直减弱的现象。     

Photoluminescence quenching of CdTe/CdS core-shell quantum dots in aqueous solution by ZnO nanocrystals

Photoluminescence (PL) properties of 3-mercaptopropionic acid (MPA) coated CdTe/CdS core-shell quantum dots (QDs) in aqueous solution in the presence of ZnO colloidal nanocrystals were studied by steady-state and time-resolved PL spectroscopy. The PL quenching of CdTe/CdS core-shell QDs with addition of purified ZnO nanocrystals resulted in a decrease in PL lifetime and a small red shift of the PL band. It was found that CdTe(1.5 nm)/CdS type II core-shell QDs exhibited higher efficiency of PL quenching than the CdTe(3.0 nm)/CdS type I core-shell QDs, indicating an electron transfer process from CdTe/CdS core-shell QDs to ZnO nanocrystals. The experimental results indicated that the efficient electron transfer process from CdTe/CdS core-shell QDs to ZnO nanocrystals could be controlled by changing the CdTe core size on the basis of the quantum confinement effect.     

Synthesis and Optical Characterization of CdS Nanowires by Chemical Process

Cadmium sulfide (CdS) nanostructured materials were synthesized by a wet chemical route without using any capping agent. X-ray diffraction pattern showed the typical interplanar spacings corresponding to the cubic phase of CdS. Transmission electron microscopy studies showed the nanowires formation with length in the range 0.1–1.5 μm and the diameter 25–30 nm. UV–visible optical spectroscopy study was carried out to determine the bandgap of the nanostructured CdS thin films and it showed blue shift with respect to the bulk value. Variation of band gap energies with annealing temperature was also studied in detail. Room temperature photoluminescence of the nano-CdS films was measured and the spectrum showed a broad band centered at ~567 nm, which originated from trap states existing in the forbidden energy gap.