水热法生长方式对ZnO纳米棒阵列结构和性能的影响

本文系统地比较了三种方式制备的ZnO纳米棒阵列的结构和性能的异同.根据水热法生长液中碱来源的不同,ZnO纳米棒阵列的生长方式分为三种:N方式(氨水)、H方式(六次甲基四胺)和NH方式(两次N方式和一次H方式).通过扫描电子显微镜,对这三种方式生长的ZnO纳米棒阵列形貌进行了表征.此外,利用X射线衍射仪、透射电子显微镜和激光拉曼光谱对ZnO的结晶性能进行比较.结果表明,ZnO纳米棒阵列的取向性N≈NH>H,ZnO的晶体质量H>NH>N.NH方式综合N方式和H方式的优势,得到了取向性和晶体质量优良的ZnO纳米棒阵列.这将为在进一步应用中有效地选择ZnO纳米棒阵列的制备方式提供重要信息.     

基底对电沉积制备ZnO纳米棒阵列的影响

采用恒电位电沉积方法, 在未经修饰的ITO导电玻璃基底上通过控制实验条件制备出不同形貌的纳米ZnO结构, 而在经过ZnO纳米粒子膜修饰后的ITO导电玻璃基底上, 制备出透明、高取向、粒径小于30 nm的ZnO纳米棒阵列. 用扫描电子显微镜(SEM)、X射线衍射(XRD)以及透射光谱对制备出的ZnO纳米棒阵列的结构、形貌和透明性进行了表征. 测试结果表明, ZnO纳米棒阵列的平均直径为21 nm, 粒径分布窄, 约18～25 nm, 择优生长取向为[001]方向, 垂直于基底生长. 当入射光波长大于400 nm时, ZnO纳米棒阵列的透光率大于95%.     

ZnO纳米棒阵列的同步法制备及其PL性能研究

在较低温度下，采用化学法在Zn片和玻璃片上同步制备了ZnO纳米棒阵列。利用XRD、FESEM和HRTEM对样品进行了表征，并且通过光致发光谱研究了阵列的光致发光(PL)性能。结果表明，ZnO纳米棒阵列较为致密、取向性较好。纳米棒为六方纤锌矿相，沿c轴生长，平均直径约为60 nm。同步法制备的2种ZnO纳米棒阵列均具有较好的紫外和橙红色发光性能，但发光特性却存在一定差异，这可能主要是由于2种阵列中纳米棒的缺陷含量不同所致。     

一维有序ZnO纳米棒阵列的制备和优化

以氧化铟锡透明导电膜玻璃(ITO)做载体,先在室温下采用浸渍-提拉法制备出ZnO纳米晶作为种子层,再结合低成本的水热生长法合成了一维有序的ZnO纳米棒阵列.结合X射线衍射(XRD)、扫描电子显微镜(SEM)和能量色散谱仪(EDS)表征,研究了前驱液浓度、溶胶陈化时间、种子层提拉次数、水热生长时间和次数等5种因素对ZnO纳米棒的结构及形貌的影响.研究结果表明, ZnO纳米棒阵列的长度和直径会随着前驱液的浓度和溶胶陈化时间以及水热生长时间的延长而增加.当前驱液浓度为0.5 mol·L^-1时,陈化时间为24 h,浸渍-提拉3次,水热反应3次,每次反应时间为150 min时,可得到一维有序的ZnO纳米棒阵列.     

电沉积ZnO纳米棒阵列膜制备及其透光性能研究

应用阴极恒电流电沉积法,以ZnC l2水溶液为电解液,在经预处理的ITO导电玻璃上制备ZnO纳米棒阵列,扫描电子显微镜(SEM)、X射线衍射(XRD)及透射光谱等测试表明,ZnO纳米棒阵列具有c轴高度择优取向,呈六方纤锌矿结构.当入射光波长大于380 nm时,ZnO纳米棒阵列的透光率大于95%,并且禁带宽度变窄.     

表面修饰引发的ZnO纳米棒阵列膜的超疏水性

润湿性是固体表面的重要性质之一 ,它受控于固体表面自由能和表面粗糙度的大小 ,一般可用液体在固体表面接触角的大小来衡量 .由于水与超疏水表面 (水与固体表面的接触角大于 1 5 0°的表面 )的接触面积很小 ,通过水所发生的化学发应和化学键的形成受到限制 ,使这种表面具有防水、防污染和防氧化等多种功能 ,因而备受人们的关注 [1～ 6 ] .作为宽禁带半导体材料 ,Zn O以其独特的光电和催化等性质在短波激光器、气体传感器、高效催化剂、太阳能电池等方面具有广阔的应用前景 .表面润湿性的研究对于将 Zn O用于各种器件非常重要 .Pesika等 […     

水热法制备高度取向的氧化锌纳米棒阵列

氧化锌的激子结合能(60meV)及光增益系数(300cm^-1)比GaN的(25meV,100cm^-1)还高,这一特点使它成为紫外半导体激光发射材料的研究热点。最近,Yang等成功地观测到规则的ZnO纳米线阵列的激光发射现象,更加激起了人们合成一维高度有序ZnO纳米结构的热情,由于一维ZnO     

低温一步液相法合成ZnO纳米棒

近年来．一维纳米结构如纳米线、纳米棒、纳米带等．由于其新颖的物理化学性质及其在光学或电学器件上的广泛应用前景．已成为研究开发的热点。特别是氧化锌（ZnO）这种宽禁带（3．37eV）、高激子束缚能（60meV）的功能性半导体材料。基于它在光电子器件、太阳能电池、传感器、二极管、场发射显示器等领域潜在的重要应用价值，各国科学工作者都给予极大的研究热情．开发出了许多合成方案制备一维纳米ZnO结构，如水热法，模板法同，微乳液法阐，CVD法，热蒸发法，MOVPE法，电化学沉积法等。     

氧化锌纳米棒的水热合成及其光催化性能

以分析纯ZnO作为锌源、NaOH为矿化剂、盐酸为反应溶液pH调节剂,利用水热反应制备了花状ZnO纳米棒;采用扫描电子显微镜和X射线衍射仪分析了产物的形貌和结构,考察了水热温度以及Zn2+和OH-浓度比对产物形貌的影响;以甲基橙为目标降解物,采用紫外-可见分光光度计研究了ZnO纳米棒的光催化性能.结果表明,在水热反应温度80℃、Zn2+/OH-浓度比1∶7.5条件下所得ZnO纳米棒呈花状聚合,直径约为200nm,长度约为2μm,具有六方纤锌矿结构.当甲基橙初始浓度为30 mg.L-1、ZnO纳米棒的投放量为1.5g.L-1时,以300W紫外灯照射150min,甲基橙的降解率可达90%.     

ZnO/ZnS Heterostructured Nanorod Arrays and Their Efficient Photocatalytic Hydrogen Evolution

Semiconducting heterostructures have been widely applied in photocatalytic hydrogen evolution due to their variable band gaps and high energy conversion efficiency. As typical semiconducting heterostructures, ZnO/ZnS heterostructured nanorod arrays (HNRAs) have been obtained through a simple anion‐exchange process in this work. Structural characterization indicates that the heterostructured nanorods (HNRs) are all composed of hexagonal wurtzite ZnO core and cubic zinc‐blende ZnS shell. As expected, the as‐obtained one‐dimensional heterostructures not only lower the energy barrier but also enhance the separation ability of photogenerated carriers in photocatalytic hydrogen evolution. Through comparisons, it is found that 1D ZnO/ZnS HNRAs exhibit much better performance in photocatalytic hydrogen evolution than 1D ZnO nanorod arrays (NRAs) and 1D ZnS NRAs. The maximum H₂ production is 19.2 mmol h^?1 for 0.05 g catalyst under solar‐simulated light irradiation at 25 °C and the corresponding quantum efficiency is 13.9 %, which goes beyond the economical threshold of photocatalytic hydrogen evolution technology.     

Ti基ZnO纳米棒阵列的制备及其光催化性能研究

采用两电极体系中恒电流电沉积在Ti基底上制得较均一的ZnO纳米棒阵列,利用SEM和XRD观察表征样品,研究Zn(NO₃)₂浓度及电流密度对ZnO纳米棒阵列微观形貌的影响. 以甲基橙为目标降解物,考察该电极光催化性能. 结果表明,Zn(NO₃)₂浓度和电流密度对纳米棒阵列的形貌有显著影响;与ITO玻璃等其他基底相比,在Ti基底上也可沉积较好均一取向的ZnO纳米棒阵列;紫外灯照射下,ZnO/Ti电极对甲基橙（10 mg·L^-1）模拟印染废水降解2.5 h,降解率达到83.3%,光催化活性较佳;无光照时ZnO纳米棒的降解率仅7%.     

特定条件下的定向ZnO纳米棒的制备及表征

采用改进的溶胶凝胶和化学溶液生长两步法, 并控制特定条件在镀银载玻片上制备出定向ZnO纳米棒. 利用X射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)、选区电子衍射(SAED)、能谱(EDS)及傅里叶红外吸收光谱(FTIR)对纳米棒的表面形貌、结构、组分进行分析. XRD和SEM结果表明该ZnO纳米棒具有六角纤锌矿结构, 结晶质量良好, 垂直衬底生长. TEM和SAED结果表明该ZnO纳米棒形状规则, 为单晶结构. FTIR谱中的位于418 和541 cm^－1的吸收峰对应于棒状ZnO结构的伸缩振动吸收峰, 1384 和1636 cm^－1对应于六方纤锌矿ZnO晶体的Zn—O伸缩振动吸收峰. 利用负离子配位四面体生长理论初步解释ZnO纳米棒的生长过程.     

ZnO纳米棒阵列基-芴类共轭聚合物膜的制备及对TNT的检测评价

将共轭芴类荧光聚合物涂覆在纳米Zn O棒阵列上,制成荧光传感膜检测痕量TNT。通过水热法生长的Zn O纳米棒阵列具有较好的取向性,作为衬底可有效增大荧光膜荧光强度,同时,Zn O纳米棒阵列的高比表面积可提高膜对TNT气体的响应效率,使20s内的荧光猝灭率可达72%。     

Hydrothermal growth of well-aligned ZnO nanorod arrays: Dependence of morphology and alignment ordering upon preparing conditions

Well-aligned ZnO nanorod arrays were prepared on substrates by hydrothermal growth under different conditions. The effect of preparing conditions on the deposition of ZnO nanorods was systematically studied by scanning electron microscopy, X-ray diffraction and photoluminescence spectroscopy. It is demonstrated that the growth conditions such as pre-treatment of the substrates, growth temperature, deposition time and the concentration of the precursors have great influence on the morphology and the alignment ordering of ZnO nanorod arrays. Pre-treatment of substrates, including dispersion of ZnO nanoparticles and subsequent annealing, not only plays a main role in governing the rod diameter, but also greatly improves the rod orientation. Although the rod diameter and its distribution are mainly determined by pre-coated ZnO nanoparticles, they can also be monitored to some extent by changing the concentration of the precursors. The growth temperature has a little influence on the orientation of nanorods but it has great impact on their aspect ratio and the photoluminescent property. Kinetic studies show that the growth of ZnO nanorods contains two distinct step: a fast steps within the first hour, in which the nanorods tend to be short and wide, and a slow step, in which long rods with high aspect ratio are obtained.     

A Study on the Influences of Processing Parameters on the Growth of Oxide Nanorod Arrays by Sol Electrophoretic Deposition

Template-based sol electrophoretic deposition has been demonstrated as an attractive method for the synthesis of oxide nanorod arrays, including simple and complex oxides in the forms of amorphous, polycrystalline, and single crystal. This paper systematically studied a number of processing parameters to control nanorod growth by sol electrophoretic deposition. The influences of particle and template zeta potentials, condensation rate, deposition rate (or externally applied electric field), the presence of organic additives, and sol concentration on the growth of nanorod arrays were studied. It was found that higher zeta potential or electric field resulted in higher growth rates but less dense packing. Templates with charge opposite to that of the sol particles prevented formation of dense nanorods, sometimes resulting in nanotubes, depending on the field strength during electrophoresis. In addition, the pH of the sol and chelating additives were also varied and likely affected the deposition process by affecting the condensation reactions.     

高度有序氧化钨纳米棒的制备和表征

采用直流磁控溅射法结合阳极氧化法在铝基纳米点阵上制备氧化钨(WO3)纳米棒. 运用原子力学显微镜(AFM), 电子扫描显微镜(SEM), X射线衍射仪(XRD), 电化学工作站(EW)和紫外-可见分光光度计(UV)观察表征了WO3纳米棒的表面形貌、结构、光学性能和电致变色性能. 结果表明: 在溅射过程中, 溅射粒子优先沉积于铝基纳米点阵的凸点上, 然后成核并形成棒状; WO3纳米棒的直径约为200 nm, 与铝基纳米点阵的直径一致, 拥有一定的电致变色性能.     

Template-Based Growth of Oxide Nanorod Arrays by Centrifugation

This paper reports template-based growth of nanorod arrays by combination of sol–gel processing and centrifugation. The technical concept is simple and straightforward; centrifugation force drives the sol nanoclusters into the pores of the template, filling the pores completely to form nanorods. However, simulation reveals the formation of nanorods inside pores is more complex; centrifugation force is insufficient to overcome the energy barrier that prevents agglomeration of two nanoclusters. Thermal fluctuation and solvent evaporation upon drying are considered to be the forces leading to the eventual agglomeration of concentrated nanoclusters inside template pores. Dense nanorods with 200 nm diameter and 10 m length were readily obtained from polymeric SiO₂, colloidal SiO₂, TiO₂ and PZT sols after heat treatment.