同轴静电纺丝技术制备ZnO@CeO2纳米电缆

采用同轴静电纺丝技术,以硝酸铈、硝酸锌、聚乙烯吡咯烷酮、N,N-二甲基甲酰胺、甘油和氯仿为原料,制备了ZnO@CeO2 同轴纳米电缆。用差热–热重分析、X射线衍射、扫描电镜、透射电镜和能谱仪对样品进行了表征。结果表明,所得到的产物为ZnO@CeO2同轴纳米电缆,以晶态CeO2为壳层,晶态ZnO为芯层,电缆直径约90 nm,芯层直径约60 nm,壳层厚度约15 nm,电缆长度>300 μm,对其形成机理进行了分析。     

同轴三层纳米电缆NiO@SiO2@TiO2的制备与表征

采用静电纺丝技术, 通过改进实验装置, 成功地制备出了NiO@SiO₂@TiO₂同轴三层纳米电缆. 采用差热-热重(TG-DTA)分析、X射线衍射(XRD)分析、傅立叶变换红外光谱(FTIR)分析、扫描电子显微镜(SEM)分析和透射电子显微镜(TEM)等分析技术对样品进行表征, 结果表明, 所得产物为NiO@SiO₂@TiO₂同轴三层纳米电缆, 内层为NiO, 直径大约为40～50 nm|中间层为SiO₂, 厚度大约为40～45 nm|外层为TiO₂, 厚度大约为45～50 nm. 对NiO@SiO₂@TiO₂同轴三层纳米电缆的形成机理进行了讨论.     

同轴静电纺丝技术制备Y_2O_3:Eu~(3+)@SiO_2豆角状纳米电缆与表征

采用同轴静电纺丝技术,以氧化钇、氧化铕、正硅酸乙酯(C8H20O4Si)、无水乙醇、PVP和DMF为原料,成功制备出大量的Y2O3:Eu3+@SiO2豆角状纳米电缆.用TG-DTA,XRD,SEM,TEM和荧光光谱等分析技术对样品进行了系统地表征.结果表明,得到的产物为Y2O3:Eu3+@SiO2豆角状纳米电缆,以无定型SiO2为壳层,晶态Y2O3:Eu3+球为芯,电缆直径约为200nm,内部球平均直径约150nm,壳层厚度约为25nm,电缆长度300μm.纳米电缆内部为球状结构,沿着纤维长度方向有序排列,形貌均一.Y2O3:Eu3+@SiO2豆角状纳米电缆在246nm紫外光激发下,发射出Eu3+离子特征的波长为614nm的明亮红光.对其形成机理进行了初步讨论.     

静电纺丝技术制备NiO@Al2O3@TiO2同轴三层亚微米电缆及其形成机理

采用静电纺丝技术,通过改进实验装置,采用同轴三喷嘴实验装置代替传统的单喷嘴实验装置,在最佳的纺丝条件下制备了[Ni(CH3COO)2+PVP]@[Al(NO3)3+PVP]@[Ti(OC4H9)4+CH3COOH+PVP]前驱体复合电缆,将其进行热处理,制备出了NiO@Al2O3@TiO2同轴三层纳米电缆. 采用差热-热重(TG-DTA)、X射线衍射(XRD)、傅立叶变换红外光谱(FTIR)、扫描电子显微镜(SEM)和透射电子显微镜(TEM)等分析技术对样品进行了表征. 结果表明,所得产物为NiO@Al2O3@TiO2同轴三层纳米电缆. 纳米电缆芯层为NiO,直径大约为137.83±8.85 nm;中间层为Al2O3,厚度大约为215.11±8.66 nm;壳层为TiO2,厚度大约为156.26±16.50 nm. 对NiO@Al2O3@TiO2同轴三层纳米电缆的形成机理进行了讨论.     

Ag/C同轴纳米电缆的制备

采用十六烷基三甲基溴化铵(CTAB)辅助水热法合成了Ag/C同轴纳米电缆,并用SEM、TEM、XRD和EDS对产物进行了表征。结果表明,产物为长达数十微米,内核直径80～100 nm,壳厚约100 nm的纳米电缆。初步探讨了Ag/C同轴纳米电缆的生长机制。     

NiO@SnO2@Zn2TiO4@TiO2同轴四层纳米电缆的制备、表征及形成机理研究

采用静电纺丝技术, 通过改进实验装置, 在最佳的纺丝条件下制备了[Ni(CH₃COO)₂＋PVP]@[SnCl₄＋PVP]@[Zn(CH₃COO)₂＋PVP]@[Ti(OC₄H₉)₄＋CH₃COOH＋PVP]前驱体复合电缆, 将其进行热处理, 制备出NiO@ SnO₂@Zn₂TiO₄@TiO₂同轴四层纳米电缆. 采用热重-差热(TG-DTA)、X射线衍射(XRD)、傅立叶变换红外光谱(FTIR)、扫描电子显微镜(SEM)和透射电子显微镜(TEM)等分析技术对样品进行了表征. 结果表明, 所得产物为同轴四层纳米电缆, 芯层为NiO, 直径为35～55 nm|第二层为SnO₂, 厚度为30～50 nm|第三层为Zn₂TiO₄, 厚度为25～40 nm|壳层为TiO₂, 厚度为40～90 nm. 对同轴四层纳米电缆的形成机理进行了探讨.     

同轴静电纺丝技术制备Y2O3:Eu3＋@SiO2豆角状纳米电缆与表征

采用同轴静电纺丝技术, 以氧化钇、氧化铕、正硅酸乙酯(C₈H₂₀O₄Si)、无水乙醇、PVP和DMF为原料, 成功制备出大量的Y₂O₃:Eu^3＋@SiO₂豆角状纳米电缆. 用TG-DTA, XRD, SEM, TEM和荧光光谱等分析技术对样品进行了系统地表征． 结果表明, 得到的产物为Y₂O₃:Eu^3＋@SiO₂豆角状纳米电缆, 以无定型SiO₂为壳层, 晶态Y₂O₃:Eu^3＋球为芯, 电缆直径约为200 nm, 内部球平均直径约150 nm, 壳层厚度约为25 nm, 电缆长度＞300 μm. 纳米电缆内部为球状结构, 沿着纤维长度方向有序排列, 形貌均一. Y₂O₃:Eu^3＋@SiO₂豆角状纳米电缆在246 nm紫外光激发下, 发射出Eu^3＋离子特征的波长为614 nm的明亮红光. 对其形成机理进行了初步讨论.     

用离子吸附法制备银/聚吡咯同轴纳米电缆

以多元醇还原反应法制备出直径为40~50 nm的纳米银线, 采用醋酸铜水溶液对银纳米线表面进行处理, 通过离子吸附在纳米银线表面吸附铜离子. 以吸附在银纳米线表面上的铜离子作为活性单元, 氧化吡咯单体聚合, 制得Ag/PPy同轴纳米电缆. 采用TEM, FTIR和XPS等表征手段对产物进行表征和检测, 并通过表面增强拉曼光谱进一步证实产物中聚吡咯层紧密地吸附在银线表面. 结果表明, 利用醋酸铜作为氧化剂, 通过离子吸附法制备的Ag/PPy同轴纳米电缆, 可以在较大范围内有效地控制聚吡咯层厚度, 避免银纳米线被刻蚀.     

铟掺杂氧化锌-氧化硅纳米电缆芯-壳异质结构的制备及表征

利用碳热还原反应气相沉积法制备了铟掺杂氧化锌-氧化硅纳米电缆芯-壳异质结构. X射线衍射(XRD)、透射电子显微镜(TEM)及X射线能谱(EDS)研究表明, 纳米电缆内芯为结晶完好的单晶纤锌矿结构, 外壳包覆一层氧化硅非晶层. 纳米电缆直径为30-60 nm, 长径比大于100. 掺杂纳米异质结构的生长机理与传统的金属晶种辅助气-液-固(VLS)机理有所不同. 这种掺杂纳米异质结构有望作为理想的结构单元应用于纳米器件领域.     

同轴静电纺丝法制备ZnO/Ag2O纳米纤维材料及其光电催化性能研究

以醋酸锌和乙酰丙酮银为前驱体, 通过同轴静电纺丝和热处理过程在氟掺杂氧化锡(FTO)导电玻璃上制备了ZnO/Ag₂O同轴纳米纤维. 采用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)、 拉曼光谱和紫外-可见漫反射光谱(UV-Vis DRS)等手段对材料进行了表征. 以氙灯模拟可见光光源, 亚甲基蓝为目标降解物, 考察了所制备纳米纤维的光电催化活性. 结果表明, 同轴ZnO/Ag₂O纳米纤维具有壳核类似结构(ZnO为壳, Ag₂O为核), Ag₂O与ZnO形成的异质结和杂质能级降低了ZnO的带隙能, 提高了对可见光的利用率. 在可见光下, 与纯ZnO相比, ZnO/Ag₂O具有很强的光电催化能力, 并且Ag₂O的量对同轴纤维光电催化活性影响很大, 在同样光电催化条件下, ZnO/Ag₂O-7同轴纳米纤维的光电催化效果最好, 亚甲基蓝降解率达93%, 动力学常数最大为1.13×10 ^-2 min ^-1.     

Preparation and Characterization of Polypyrrole/TiO2 Coaxial Nanocables

Summary: We demonstrate in this communication that large‐scale coaxial nanocables of polypyrrole (PPy)/TiO₂ can be obtained via three steps: (1) synthesis of TiO₂ nanofibers by electrospinning; (2) physical adsorption Fe³⁺ oxidant on the surface of TiO₂ nanofibers; (3) followed by polymerization of pyrrole (from vapor) on the surface of TiO₂ nanofibers. During the synthesis, the PPy formed on TiO₂ nanofibers as a template and formed PPy/TiO₂ coaxial nanocables. TEM image proved that PPy (20 nm thickness) covered the surface of TiO₂ nanofibers. Fourier‐transform infrared (FTIR), X‐ray photoelectron spectra (XPS), and X‐ray diffraction patterns (XRD) characterized the chemical structure of the coaxial nanocables. Surface photovoltage spectroscopy (SPS) revealed the surface properties of the PPy/TiO₂ coaxial nanocables.

TEM image of individual PPy/TiO₂ coaxial nanocable.     

Aligned Zn-Zn2SiO4 core-shell nanocables with homogeneously intense ultraviolet emission at 300 nm

Aligned coaxial nanocables were grown on Si substrates by a vapor-deposition technique. The lengths of the nanocables increased as the distance between the substrate and the source decreased. The nanocables were characterized as homogeneously crystallized shells of about 25 nm thick, diameters of about 100 nm, and round top ends. It was found that the shell emits an intense middle-ultraviolet about 300 nm at room temperature. This emission was attributed to the thin double-layer structure in the Zn-Zn2SiO4 core-shell nanocable where the Zn2SiO4 shell has the potential to serve as more ideal luminophors. The results demonstrated that the nanocable density could be changed by altering nucleation density at the steps on the substrate surface. The unique growth manner described herein provides a new technique for the homogeneous crystallization of Zn-Zn2SiO4 core-shell nanocables.     

Preparation of highly conductive, self-assembled gold/polyaniline nanocables and polyaniline nanotubes

One-dimensional gold/polyaniline (Au/PANI-CSA) coaxial nanocables with an average diameter of 50-60 nm and lengths of more than 1 mum were successfully synthesized by reacting aniline monomer with chlorauric acid (HAuCl(4)) through a self-assembly process in the presence of D-camphor-10-sulfonic acid (CSA), which acts as both a dopant and surfactant. It was found that the formation probability and the size of the Au/PANI-CSA nanocables depends on the molar ratio of aniline to HAuCl(4) and the concentration of CSA, respectively. A synergistic growth mechanism was proposed to interpret the formation of the Au/PANI-CSA nanocables. The directly measured conductivity of a single gold/polyaniline nanocable was found to be high (approximately 77.2 S cm(-1)). Hollow PANI-CSA nanotubes, with an average diameter of 50-60 nm, were also obtained successfully by dissolving the Au nanowire core of the Au/PANI-CSA nanocables.     

Manipulation of the morphology of semiconductor-based nanostructures from core-shell nanoparticles to nanocables: the case of CdSe/SiO(2)

The morphology of CdSe/SiO(2) was manipulated from core-shell-structured nanoparticles to nanocables by using a chemical vapor deposition (CVD) process. The growth of nanocables, with cores no more than 20 nm in diameter, is initiated by the formation of core-shell nanoparticles with SiO(2) as matrix and CdSe clusters dispersed inside. After the subsequent vaporization of the SiO(2) matrix, the follow-up CdSe vapor crystallizes with the remaining CdSe clusters as nuclei to form CdSe nanowires as the furnace was cooled to 1200 degrees C. During the controlled cooling of the furnace, the SiO vapor re-deposits to sheathe the nanowires. The thickness of the shell and the diameter of core were successfully controlled. The photoluminescence measurements show that the CdSe/SiO(2) nanocables have strong visible-light emission bands located at 590 and 688 nm, which are attributed to the defects induced by SiO(2) sheaths nanowires and the quantum confinement effect of the CdSe, respectively. The UV/Vis absorption spectra of the naked CdSe nanowires further validate the above-mentioned quantum confinement effect. The deterministic growth of these nanocables is very important for the design of the nanodevices based on them.     

CNT@Fe3O4@C Coaxial Nanocables: One‐Pot,Additive‐Free Synthesis and Remarkable Lithium Storage Behavior

By using carbon nanotubes (CNTs) as a shape template and glucose as a carbon precursor and structure‐directing agent, CNT@Fe₃O₄@C porous core/sheath coaxial nanocables have been synthesized by a simple one‐pot hydrothermal process. Neither a surfactant/ligand nor a CNT pretreatment is needed in the synthetic process. A possible growth mechanism governing the formation of this nanostructure is discussed. When used as an anode material of lithium‐ion batteries, the CNT@Fe₃O₄@C nanocables show significantly enhanced cycling performance, high rate capability, and high Coulombic efficiency compared with pure Fe₂O₃ particles and Fe₃O₄/CNT composites. The CNT@Fe₃O₄@C nanocables deliver a reversible capacity of 1290 mA h g^?1 after 80 cycles at a current density of 200 mA g^?1, and maintain a reversible capacity of 690 mA h g^?1 after 200 cycles at a current density of 2000 mA g^?1. The improved lithium storage behavior can be attributed to the synergistic effect of the high electronic conductivity support and the inner CNT/outer carbon buffering matrix.     

三层同轴静电纺丝技术制备TiO2@SiO2同轴双壁亚微米管及光催化性能研究

采用三层同轴静电纺丝技术,以钛酸丁酯、正硅酸乙酯、聚乙烯吡咯烷酮、无水乙醇、芝麻油、山梨糖醇酐油酸酯和氯仿为原料,成功制备出TiO2@SiO2同轴双壁亚微米管.用差热–热重分析、X射线衍射、红外光谱仪、扫描电镜、透射电镜和能谱仪对样品进行了表征.结果表明,得到的产物为TiO2@SiO2同轴双壁亚微米管,以非晶态SiO2为外壳,晶态金红石型TiO2为内壁,同轴双壁亚微米管平均直径约680 nm,管壁厚约70 nm、内壁厚约40 nm、外壳厚约30 nm,长度大于20μm,对其形成机理进行了分析.同轴双壁亚微米管对罗丹明B显示了较好的光催化活性.