铁镍合金纳米管阵列的模板制备和磁性

"在阳极氧化铝模板的孔洞中利用模板浸润的方法成功制备出了铁镍合金纳米管阵列．通过改变所用模板的参数和沉积纳米管的的制备条件,所制备的纳米管的长度、内径和外径的尺寸都可以得到有效控制．利用扫描电子显微镜和透射电子显微镜对所制备的纳米管及其阵列的形貌进行了表征．对铁镍合金纳米管阵列的宏观磁性测量表明样品具有磁各向异性,沿纳米管长轴方向样品更容易被磁化．对纳米管的磁化反转机制和磁矩在纳米管中的静态分布进行了讨论．铁镍合金纳米管的这些性质都是由纳米管的独特结构造成的．"     

硼碳氮纳米管的热解法制备及生长机理研究

以乙二胺、二茂铁和硼氢化钠为原料,以N2和H2为辅气,用钴作催化剂,在不同温度下制备出了具有竹节状结构的硼碳氮(BCN)纳米管.根据透射电子显微镜观察,分析了BCN纳米管的生长机理.B和N的同时掺杂,所形成的五边形结构比单独N掺杂时具有更低的形成能,是竹节状结构形成的主要原因.用Raman光谱可以用来表征BCN纳米管中B和N的掺杂程度及纳米管的质量.分析表明,在860℃下制备的BCN纳米管竹节状结构最密集,质量最好,产率最高.扫描俄歇微探针分析表明,在860℃下制备的BCN纳米管的元素组成比为B∶N∶C= 关键词： BCN纳米管 热解 透射电子显微镜 Raman光谱     

不同氮源制备CNx纳米管薄膜及其低场致电子发射性能

采用高温热解法,分别以氯化铵(NH4Cl)和乙二胺(C2H8N2)为氮源在洁净的硅片上沉积生长CNx纳米管薄膜.利用扫描电子显微镜、高分辨率透射电子显微镜和拉曼光谱对CNx纳米管进行形貌观察和表征.结果显示不同氮源制备出的CNx纳米管薄膜的洁净度、有序度以及纳米管的结构明显不同.热解乙二胺(C2H8N2)/二茂铁(C10H10Fe)制备出的结晶度较低的"竹节状"结构CNx纳米管平行基底表面有序生长,而且低场致电子发射性能优越,开启电场1.0V/μm,外加电场达到2.89V/μm时发射电流密度为860μA/cm2.     

生长在Si基底上VO_x纳米管形貌的时间影响因子及其气敏性初探

采用水热法成功制备了在Si基底上的钒氧化物纳米管.通过X射线衍射、拉曼光谱、扫描电子显微镜对纳米管的结构和形貌进行了表征,测试了在不同的搅拌时间和水热反应时间下纳米管形貌的变化以及气敏性质.着重探讨了不同的搅拌时间和水热反应时间对样品形貌和气敏特性的影响.结果表明,水热反应时间越长,样品管状形貌越好,边缘越平滑.其气敏敏感度越好,响应时间也比水热反应时间短的样品要快.VO_X纳米管内径分布在25—35 nm,外径分布在65—100 nm.     

CNx纳米管的制备、结构观察及低场致电子发射性能研究

采用高温热解法 ,以乙二胺为前驱液 ,在沉积有铁催化剂的p型硅 (1 1 1 )基底上制备出了定向生长的CNx 纳米管 .利用扫描电子显微镜、高分辨率透射电子显微镜和拉曼光谱对CNx 纳米管进行了形貌观察和表征 .CNx 纳米管的高度在 2 0 μm左右 ,直径在 5 0— 1 0 0nm之间 ,具有明显的“竹节状”结构 ,结晶有序度较差 .对CNx 纳米管薄膜进行低场致发射性能测试 :外加电场为 1 4V μm ,观察到 2 0 μA cm2 发射电流 ,外电场升至 2 5 4V μm时发射电流达到1 2 80mA cm2 ,在较高外电场下 ,没有发现电流“饱和” .这比相同实验条件下改变前驱液制备出的碳纳米管和硼碳氮纳米管的场发射性能优越 .还在“竹节状”结构的基础上对CNx 纳米管的场致电子发射机理进行了讨论     

模板合成法制备TiO2:Eu3+纳米管及其发光特性研究

以碳纳米管做模板,在不利用任何表面活性剂或催化剂情况下,通过溶剂热法成功合成均匀的TiO2:Eu3+纳米管。X射线衍射结果表明,该产物是TiO2的一种纯锐钛矿相。扫描电子显微镜及透射电子显微镜图像显示,所得到的TiO2:Eu3+纳米管在大小及分布上是均匀的,管壁的厚度约为8nm。提出了该纳米管可能的形成机制。发光光谱表明,由于5D0→7F2间的转换,TiO2:Eu3+纳米管会在612nm发出红光。此外,因为制备容易而且成本较低,这种合成路径还有望用来制备其他的一维无机纳米材料。     

模板合成法制备TiO2:Eu3+纳米管及其发光特性研究

以碳纳米管做模板,在不利用任何表面活性剂或催化剂情况下,通过溶剂热法成功合成均匀的TiO2:Eu3+纳米管。X射线衍射结果表明,该产物是TiO2的一种纯锐钛矿相。扫描电子显微镜及透射电子显微镜图像显示,所得到的TiO2:Eu3+纳米管在大小及分布上是均匀的,管壁的厚度约为8nm。提出了该纳米管可能的形成机制。发光光谱表明,由于5D0→7F2间的转换,TiO2:Eu3+纳米管会在612nm发出红光。此外,因为制备容易而且成本较低,这种合成路径还有望用来制备其他的一维无机纳米材料。     

不同氮源制备CNx纳米管薄膜及其低场致电子发射性能

采用高温热解法，分别以氯化铵(NH₄Cl)和乙二胺(C₂H₈N₂)为氮源在洁净的硅片上沉积生长CN_x纳米管薄膜.利用扫描电子显微镜、高分辨率透射电子显微镜和拉曼光谱对CN_x纳米管进行形貌观察和表征.结果显示不同氮源制备出的CN_x纳米管薄膜的洁净度、有序度以及纳米管的结构明显不同.热解乙二胺(C₂H₈N₂)/二茂铁(C₁₀H₁₀Fe)制备出的结晶度较低的“竹节状” 结构CN_x纳米管平行基底表面有序生长，而且低场致电子发射性能优越,开启电场1.0V/μm，外加电场达到2.89V/μm时发射电流密度为860μA/cm². 关键词： x纳米管')" href="#">CN_x纳米管 高温热解 “竹节状”结构 场致发射     

水热合成钛酸盐纳米管及其光催化性能研究

本文采用水热法制备了钛酸盐纳米管,并用X射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)和紫外-可见光谱(UV-VIS)对样品进行了分析。以罗丹明B溶液为目标降解物,考察了样品的光催化性能。结果表明纳米管管径在8～20纳米之间,管长从几百纳米到几微米,具有不同于锐钛矿的钛酸盐结构。在紫外光照射下,钛酸盐纳米管的光催化性能明显高于TiO2纳米粒子,光照100分钟后降解率达到87%。     

高度有序的TiO2纳米管在有机电解液中的制备及碳掺杂TiO2纳米管的性能

"采用电化学阳极氧化法,在含有氟离子的有机电解液中,使纯钛表面形成一层高度有序的TiO2纳米管阵列．通过控制不同的阳极氧化电压和时间,可以得到形貌不同的TiO2纳米管．最长的TiO2纳米管接近60 1m,长径比约为600．TiO2纳米管在不同的温度(450、550和650 ℃)下焙烧2 h,采用SEM、XRD、EDS和UV-Vis分光光度仪对样品进行表征．X射线衍射仪测试结果表明制备的TiO2纳米管是无定型的,当在较高的温度下焙烧时,其结构由无定型转变为锐钛型和金红石型．EDS微量分析表明TiO2纳米管中     

Large-scale and catalyst-free synthesis of zinc nanotubes and nanowires

Metallic zinc one-dimensional materials including nanotubes and nanowires were synthesized on a large scale by a simple method. The process was both catalyst and template free. The resulting Zn nanotubes and Zn nanowires were characterized and confirmed by means of X-ray diffraction, field emission scanning electron microscopy, energy dispersive X-ray spectroscopy, and transmission electron microscopy. The growth of Zn nanotubes was reported for the first time.     

Effects of synthesis methods of vanadium oxide nanotubes on the inter layer distances

Vanadium oxide nanotubes were synthesized via two methods: (1) Adding a template to vanadium oxide gels, (2) Grinding mixture of a template and vanadium oxide by using a ball mill. Influence of preparation method on structure of vanadium oxide nanotubes has been investigated. Vanadium oxide nanotubes has been characterized by X-ray diffraction (XRD), Scanning electron microscopy (SEM), and Transmission electron microscopy (TEM) techniques.     

Fe nanowire encapsulated in boron nitride nanotubes

Boron nitride (BN) nanotubes, nanohorns, nanocoils were synthesized by annealing Fe₄N and B powders at 1000 °C for 1 h in nitrogen gas atmosphere. Especially, Fe-filled BN nanotubes were produced, and investigated by high-resolution electron microscopy, high-angle annular dark-field scanning transmission electron microscopy, electron diffraction and energy dispersive X-ray spectroscopy, which indicates that the [110] of Fe is parallel to the BN nanotube axis. Formation mechanism of Fe-filled BN nanotube was speculated based on these results.     

Synthesis and characterization of Cu2ZnSnSe4 nanotube arrays on fluorine-doped tin oxide glass substrates

Highly ordered arrays of Cu₂ZnSnSe₄ nanotubes have been successfully synthesized on fluorine-doped tin oxide glass substrate using ZnO nanorod arrays as sacrificial templates. The structure, morphology and optical properties of the Cu₂ZnSnSe₄ arrays were characterized by X-ray diffraction, Raman spectrometry, field-emission scanning electron microscopy, transmission electron microscopy, energy dispersive X-ray, and UV–Vis absorption spectroscopy. The diameter and length of the Cu₂ZnSnSe₄ nanotubes can be adjusted by tuning the diameter and length of the ZnO nanorods. In addition, the effect of the length on the performance of the photoelectrochemical cells was also investigated.     

Solution synthesis of ZnO nanotubes via a template-free hydrothermal route

ZnO nanotubes were successfully synthesized by a simple template-free hydrothermal method. X-ray powder diffraction and transmission electron microscopy were used to characterize the as-prepared ZnO nanotubes. The average size of the nanotubes is 200-500 nm in length and 20-30 nm in diameter. In addition, a further investigation of the optimized synthetic conditions has been carried out.     

Template synthesis of well-aligned titanium dioxide nanotubes

TiO₂ nanotubes of the anatase form have been synthesized by sol-gel chemical method using anodic aluminum oxide (AAO) as a template. Transmission electron microscopy (TEM), scanning electron microscopy (SEM), and X-ray diffraction were used to investigate the structure and morphology of the TiO₂ nanotubes. The results showed that TiO₂ nanotubes obtained are highly ordered and uniform. The diameter and length of the obtained nanotubes were determined by the pore size and the thickness of AAO template. It was found that through control of immersion time of AAO membrane in sol, both tubules and fibrils can be prepared. PACS 61.46.+w     

Fabrication of well-aligned CdS nanotubes by CVD-template method

Well-aligned CdS nanotubes have been synthesized within the nanochannels of the porous anodic alumina (PAA) membranes by pyrolyzing cadmium bis(diethyldithiocarbamate) [Cd(S₂CNEt₂)₂] at 400 °C. Scanning electron microscopy (SEM) and transmission electron microscopy (TEM) show that the CdS nanotubes are highly ordered with uniform diameter in range of 80-150 nm and the length up to tens of microns. X-ray diffraction (XRD), Raman spectrum, energy-dispersive spectroscopy (EDS) and selected-area electron diffraction (SAED) demonstrate that the nanotubes are composed of pure hexagonal phase polycrystalline CdS. The synthetic route can, in principle, be extended to fabricate other nanotubes of a wide range of semiconductors.     

Synthesis,characterization and magnetic properties of Co<Subscript>3</Subscript>O<Subscript>4</Subscript> nanotubes

Well-aligned Co₃O₄ nanotubes were synthesized within the nanochannels of porous anodic alumina membranes using a single-source chemical vapor deposition method. Scanning electron microscopy and transmission electron microscopy showed that the Co₃O₄ nanotubes are highly ordered with uniform diameter in the range of 100–300 nm and length up to tens of microns. X-ray diffraction, the Raman spectrum, energy-dispersive spectroscopy and selected-area electron diffraction demonstrated that the nanotubes are composed of pure cubic phase polycrystalline Co₃O₄. Magnetic measurements using a SQUID magnetometer suggested the presence of a strong antiferromagnetic interaction with Weiss constant θ= -248 K. The real and imaginary parts of the ac susceptibility at f= 10 Hz had a maximum at 4.0 K, and the field dependence of the magnetization at 1.8 K showed a small hysteresis loop with a coercivity of ∼ 98 Oe. PACS 81.07.De; 81.15.Gh; 78.30.-j; 75.75.+a; 61.46.Np