花状铜锌锡硫纳米颗粒的溶剂热法制备和结构表征

以金属氯化物为金属源,硫脲为硫源,聚乙二醇和乙二醇为混合溶剂,采用溶剂热法一步合成了花状的铜锌锡硫纳米颗粒.利用X射线衍射仪,扫描电子显微镜、能谱仪、透射电子显微镜、紫外-可见分光光度计分析了铜锌锡硫纳米颗粒的物相、结构、形貌及光学性能,并初步探讨了铜锌锡硫的生长机理.结果表明,所得到的铜锌锡硫纳米颗粒具有锌黄锡矿结构,直径在500～2 000nm范围内可调,其中花状的铜锌锡硫纳米颗粒由大量厚度约25nm的纳米片构成.所制备的铜锌锡硫纳米颗粒对可见光具有明显的吸收;利用外延法推算得到其禁带宽度约为1.5eV,与太阳能电池所需的最佳禁带宽度相近,显示其有望在新一代太阳能电池中得到应用和推广.     

Cu2ZnSnS4(CZTS)纳米微球的制备及表征

为研究PVP含量对CZTS颗粒形貌以及分散性的影响,本文采用溶剂热法,以CuCl2·2H2O、Zn(Ac)2·2H2O、SnCl4·5H2O作金属源,硫脲作硫源,乙二醇为溶剂,在体系中加入不同含量的PVP,成功制备了CZTS微球。通过XRD、Raman、SEM、TEM、UVVis等方法检测分析CZTS纳米微球的物相、结构、形貌以及光学性能。结果表明:所得CZTS纳米颗粒具有锌黄锡矿结构;当体系中PVP含量为0.2 g时,颗粒分散性较好,制备的颗粒形貌为表面嵌有纳米薄片的微球,纳米片较在体系中加入0.1 g PVP更致密;光学带隙约为1.47 eV,与太阳能电池所需的最佳带隙接近。最后,对表面嵌有纳米薄片的CZTS微球可能的形成机理进行了推测。     

锂离子电池负极材料铜锌锡硫纳米颗粒的制备及其电化学性能

以金属氯化物为金属源,硫脲为硫源,聚乙二醇和乙二醇为混合溶剂,采用溶剂热法一步合成了球形的铜锌锡硫纳米颗粒.利用X射线衍射仪(XRD),扫描电子显微镜(SEM)和透射电子显微镜(TEM)分析了铜锌锡硫纳米颗粒的物相、结构、形貌;利用电池测试系统对以铜锌锡硫纳米颗粒为锂离子电池负极材料组装的锂离子电池的电化学性能进行了测试.结果表明:所得到的产物为具有锌黄锡矿结构的纯相铜锌锡硫,颗粒直径在300～500nm.铜锌锡硫纳米颗粒作为锂离子电池的负极材料具有较好的稳定性,有望在锂离子电池研究和应用中得到推广.     

Cu2ZnSnS4(CZTS)纳米微球的制备及表征

为研究PVP含量对CZTS颗粒形貌以及分散性的影响,本文采用溶剂热法,以CuCl₂·2H₂O、Zn(Ac)₂·2H₂O、SnCl₄·5H₂O作金属源,硫脲作硫源,乙二醇为溶剂,在体系中加入不同含量的PVP,成功制备了CZTS微球。通过XRD、Raman、SEM、TEM、UV-Vis等方法检测分析CZTS纳米微球的物相、结构、形貌以及光学性能。结果表明:所得CZTS纳米颗粒具有锌黄锡矿结构;当体系中PVP含量为0.2g时,颗粒分散性较好,制备的颗粒形貌为表面嵌有纳米薄片的微球,纳米片较在体系中加入0.1gPVP更致密;光学带隙约为1.47eV,与太阳能电池所需的最佳带隙接近。最后,对表面嵌有纳米薄片的CZTS微球可能的形成机理进行了推测。     

Cu2ZnSnS4纳米晶微球的制备及其表征

以乙二醇为溶剂,采用溶剂热法合成出由纳米晶组装而成的Cu2ZnSnS4(CZTS)微球。采用X射线衍射仪(XRD)、拉曼光谱仪(Raman)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、紫外-可见漫反射光谱(DRS)对所得微球的结构与成分、颗粒大小与形貌和光学性质进行了测试分析。研究结果表明:溶剂热法制得的CZTS粉体具有四方晶相结构,微球由纳米晶组装而成,对可见光有良好的吸收;随着反应时间的增加,颗粒尺寸逐渐增大,且对形貌有一定影响;此外,文中还对CZTS微球的形成机理做了推测。     

钛酸钡纳米颗粒聚集球的形成机理

采用水热法合成了具有新颖结构的钛酸钡纳米颗粒聚集球.X射线衍射(XRD)结果显示该聚集球为立方相,随着时间的延长其结晶性增强.利用扫描电子显微镜(SEM)、透射电子显微镜(TEM)、高分辨透射电子显微镜(HRTEM)和电子衍射(ED)谱研究了该纳米颗粒聚集球的生长特点.结果表明该聚集球是由5-8nm的纳米颗粒定向连接生长而成,整个聚集球对外显示类单晶的现象.聚集球的大小约为60nm,随着时间的延长有长大的趋势.X射线能谱(EDX)分析结果和Johnson-Mehl-Avrami(JMA)方程动力学模拟结果表明,在颗粒球形成初始阶段主要是Ba2+离子的扩散成核作用占主导地位.这种"扩散成核-定向生长"的形成过程揭示了钛酸钡纳米颗粒聚集球的生长机理.     

酵母菌模板法制备CeO2空心微球及其光催化性能

以酵母菌为生物模板辅助沉淀法制备了Ce O2空心微球。采用傅里叶转换红外光谱(FT-IR)、X射线衍射(XRD)、X射线光电子能谱(XPS)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)和氮气吸附-脱附等对样品进行了表征,结果表明,在600℃煅烧后得到了Ce O2空心微球,其形态与酵母菌一致为椭球体,球壳是由大小约为25 nm的Ce O2纳米颗粒组成,比表面积为22 m2·g-1,远大于未用模板制备的Ce O2微粒的比表面积。通过紫外-可见漫反射测定,得到Ce O2空心微球的禁带宽度为3.03 e V,相比于相同条件下合成的无模板Ce O2禁带宽度(3.42 e V)明显减小。室温下用模拟太阳光照射降解酸性橙7(AO 7)对样品的光催化性能进行了测试,结果表明,在照射120 min之后降解率能达到96%以上,降解效果明显高于未使用模板的Ce O2微粒。对Ce O2空心微球的形成机理进行了分析。     

Cu2ZnSnS4纳米晶的制备及其三阶非线性光学性能的研究

以乙酰丙酮铜、醋酸锌、二氯亚锡、油胺和硫粉为前驱体,采用one-pot法合成出了单分散的Cu2ZnSnS4(CZTS)纳米晶.所得样品采用X射线粉末衍射仪(XRD),能量色散谱仪(EDS),透射电子显微镜(TEM),高分辨透射电子显微镜(HRTEM),光电子能谱仪(XPS),紫外-可见光谱仪(UV-vis)和Z-扫描(Z-scan)技术对其结构组成、形貌、性能等进行了表征.结果表明:所获得的产物为四方相结构的六边形CZTS纳米颗粒,直径约为10 nm.计算出尺寸大小为10 nm,13 nm的纳米晶的三阶非线性光学折射率γ(-1.08×10-15,-9.08×10-17 m2·W-1),三阶非线性光学吸收系数β(6.5×10-9,3.69×10-11 m·W-1)以及三阶非线性光学极化率χ(3)(1.49×10-9,4.35×10-10 esu).并探讨了CZTS纳米晶可能的形成机理,及引起三阶光学非线性发生变化的原因。     

油酰吗啉溶剂体系中银铟硒纳米颗粒的形貌可控合成

以绿色环保的油酰吗啉作为硒粉的溶剂,油胺作为表面包覆剂,通过简单的液相法制备了银铟硒纳米颗粒。X射线衍射和透射电子显微镜分析测试显示AgInSe2纳米颗粒属于四方黄铜矿相结构,粒径约为16 nm的六角盘状纳米晶。紫外可见光谱分析表明所制备的AgInSe2纳米颗粒禁带宽度约为1.22 eV。考察了反应时间对AgInSe2纳米颗粒尺寸的影响,发现颗粒的尺寸随着反应时间的延长而逐渐变大。对AgInSe2纳米颗粒的生长机制进行了初步探讨,油胺的选择性吸附及材料的晶体结构被认为是决定纳米颗粒形貌的主要因素。     

酵母菌模板法制备CeO2空心微球及其光催化性能

以酵母菌为生物模板辅助沉淀法制备了CeO₂空心微球。采用傅里叶转换红外光谱(FT-IR)、X射线衍射(XRD)、X射线光电子能谱(XPS)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)和氮气吸附-脱附等对样品进行了表征,结果表明,在600 ℃煅烧后得到了CeO₂空心微球,其形态与酵母菌一致为椭球体,球壳是由大小约为25 nm的CeO₂纳米颗粒组成,比表面积为22 m²·g^-1,远大于未用模板制备的CeO₂微粒的比表面积。通过紫外-可见漫反射测定,得到CeO₂空心微球的禁带宽度为3.03 eV,相比于相同条件下合成的无模板CeO₂禁带宽度(3.42 eV)明显减小。室温下用模拟太阳光照射降解酸性橙7(AO 7)对样品的光催化性能进行了测试,结果表明,在照射120 min之后降解率能达到96%以上,降解效果明显高于未使用模板的CeO₂微粒。对CeO₂空心微球的形成机理进行了分析。     

Colloidal synthesis of wurtzite Cu2ZnSnS4 nanorods and their perpendicular assembly

The quaternary copper chalcogenide Cu(2)ZnSnS(4) is an important emerging material for the development of low-cost and sustainable solar cells. Here we report a facile solution synthesis of stoichiometric Cu(2)ZnSnS(4) in size-controlled nanorod form (11 nm × 35 nm). The monodisperse nanorods have a band gap of 1.43 eV and can be assembled into perpendicularly aligned arrays by controlled evaporation from solution.     

Template-directed synthesis of ordered single-crystalline nanowires arrays of Cu2ZnSnS4 and Cu2ZnSnSe4

Highly ordered quaternary semiconductor Cu(2)ZnSnS(4) nanowires array have been prepared via a facile solvothermal approach using anodic aluminum oxide (AAO) as a hard template. The as-prepared nanowires are uniform and single crystalline. They grow along either the crystalline [110] or [111] direction. The structure, morphology, composition, and optical absorption properties of the as-prepared Cu(2)ZnSnS(4) samples were characterized using X-ray powder diffraction, transmission electron microscopy, energy dispersive X-ray spectrometry, scanning electron microscopy, and UV-vis spectrometry. A possible formation mechanism of the nanowire arrays is proposed. Governed by similar mechanism, we show that Cu(2)ZnSnSe(4) nanowire array with similar structural characteristics can also be obtained.     

Compositionally tunable Cu2ZnSn(S(1-x)Se(x))4 nanocrystals: probing the effect of Se-inclusion in mixed chalcogenide thin films

Nanocrystals of multicomponent chalcogenides, such as Cu(2)ZnSnS(4) (CZTS), are potential building blocks for low-cost thin-film photovoltaics (PVs). CZTS PV devices with modest efficiencies have been realized through postdeposition annealing at high temperatures in Se vapor. However, little is known about the precise role of Se in the CZTS system. We report the direct solution-phase synthesis and characterization of Cu(2)ZnSn(S(1-x)Se(x))(4) nanocrystals (0 ≤ x ≤ 1) with the aim of probing the role of Se incorporation into CZTS. Our results indicate that increasing the amount of Se increases the lattice parameters, slightly decreases the band gap, and most importantly increases the electrical conductivity of the nanocrystals without a need for annealing.     

Nanocrystalline ZnO with ultraviolet luminescence

Octylamine capped ZnO nanoparticles with mean diameters in the range of 4-14 nm were obtained by thermolysis of single source metal-organic precursors. The nanocrystals were characterized by X-ray diffraction, transmission electron microscopy, and UV-visible, luminescence, and excitation spectroscopies. The nanocrystals are sufficiently defect-free to exhibit band edge luminescence. The size dependence of the changes in the band gap have been calculated by different methods and compared with the Kayanuma model.     

Continuous production of Cu2ZnSnS4 nanocrystals in a flow reactor

A procedure for the continuous production of Cu(2)ZnSnS(4) (CZTS) nanoparticles with controlled composition is presented. CZTS nanoparticles were prepared through the reaction of the metals' amino complexes with elemental sulfur in a continuous-flow reactor at moderate temperatures (300-330 °C). High-resolution transmission electron microscopy and X-ray diffraction analysis showed the nanocrystals to have a crystallographic structure compatible with that of the kesterite. Chemical characterization of the materials showed the presence of the four elements in each individual nanocrystal. Composition control was achieved by adjusting the solution flow rate through the reactor and the proper choice of the nominal precursor concentration within the flowing solution. Single-particle analysis revealed a composition distribution within each sample, which was optimized at the highest synthesis temperatures used.     

水相中CdTe纳米晶的制备及其光学性质

用不同稳定剂(巯基乙酸(TGA)、巯基丙酸(MPA)、L-半胱氨酸(L-Cys)、3-巯基-1,2-丙二醇(TG))在水相中制备了CdTe纳米晶, 并用透射电子显微镜(TEM)、X射线光电子能谱(XPS)和X射线粉末衍射(XRD)等技术对其进行了表征. 研究了不同水相合成条件对CdTe纳米晶光学性质的影响, 结果表明, n(Cd):n(Te)、溶液pH值、回流时间以及稳定剂的性质, 对纳米晶的光学性质具有显著影响. 制得的CdTe纳米晶发射峰窄且对称(半高全宽达38 nm), 用不同稳定剂制备的纳米晶发光量子效率有所不同, 用不同的激发波长对纳米晶进行激发时, 发射峰并未表现出明显的移动.     

Highly sensitive WO3 hollow-sphere gas sensors

In this paper, we describe how WO(3) hollow spheres have been synthesized in solution phase by the controlled hydrolysis of WCl(6) using novel carbon microspheres as the templates. All of the products were characterized by X-ray powder diffraction (XRD), scanning electronic microscopy (SEM), and transmission electron microscopy (TEM). The as-synthesized spheres had large diameters of about 400 nm and thin shells of about 30 nm composed of numerous small nanocrystals. Prompted by the porous structure and small crystal size of the shell wall, we constructed WO(3) hollow-sphere gas sensors and found that these sensors had good sensitivity to alcohol, acetone, CS(2), and other organic gases.