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1.
探索新的碳结构是物理、材料等学科关注的热点课题. 富勒烯分子可看成是一种零维碳结构,其独特的结构和优异的性质为构筑新碳结构提供了理想的构筑单元. 本文介绍了利用限域与高压相结合的方法,在富勒烯限域体系研究中取得的进展,包括溶剂化富勒烯、富勒烯填充单壁碳纳米管(Peapod)限域体系的高压结构转变,总结了溶剂分子等对限域富勒烯高压结构相变与新结构形成的影响. 结果对新型碳结构的设计与构筑提供了新的思路与有益参考. 相似文献
2.
以单壁碳纳米管和二茂铁为原料, 采用气相扩散法合成填充率较高的二茂铁掺杂单壁碳纳米管(Fc@SWNTs)的复合材料. 考察激光辐射对样品的影响, 结果表明, 当激光功率达到20 mW时, 对样品进行10 s辐照, 样品的拉曼光谱出现了稳定的新峰. 对比分析发现, 二茂铁在激光辐照后形成了碳化铁, 同时部分碳源转化成碳管形成了双层碳管. 表明碳化铁是二茂铁裂解向内层碳管转化的中间产物. 相似文献
3.
Raman spectra of C_(60) filled single-walled carbon nanotubes(C_(60)@SWNTs) with diameters of 1.3–1.5 nm have been studied under high pressure. A plateau in the pressure dependence of the G-band frequency at around 10 GPa was observed in both experiments with 514 nm and 830 nm excitation lasers, which is similar to the high pressure behaviors of pristine SWNTs. This structural transition has been assigned to the transformation into a peanut-like structure of the nanotubes. At pressure below 2 GPa, no obvious Raman signature related to the structural transition of nanotubes was observed, unlike what has been reported for C_(70) filled nanotubes. We discussed this point in terms of the arrangement differences of C_(60) and C_(70)molecules inside the nanotubes. At higher pressure up to 15 GPa, a graphite-like pressure evolution was observed in our C_(60)@SWNTs. 相似文献
4.
Structural Evolution of D5h(1)-C90 under High Pressure:A Mediate Allotrope of Nanocarbon from Zero-Dimensional Fullerene to One-Dimensional Nanotube
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The hybridization of fullerene and nanotube structures in newly isolated C90 with the D5 h symmetric group(D5 h(1)-C90) provides an ideal model as a mediating allotrope of nanocarbon from zero-dimensional(OD) fullerene to one-dimensional nanotube.Raman and infrared spectroscopy combined with classical molecular dynamics simulation were used to investigate the structural evolution of D5 h(1)-C90 at ambient and high pressure up to35... 相似文献
5.
Controllable synthesis of fullerene nano/microcrystals and their structural transformation induced by high pressure
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Fullerene molecules are interesting materials because of their unique structures and properties in mechanical, electrical, magnetic, and optical aspects. Current research is focusing on the construction of well-defined fullerene nano/microcrystals that possess desirable structures and morphologies. Further tuning the intermolecular interaction of the fullerene nano/microcrystals by use of pressure is an efficient way to modify their structures and properties, such as creation of nanoscale polymer structures and new hybrid materials, which expands the potential of such nanoscale materials for di- rect device components. In this paper, we review our recent progress in the construction of fullerene nanostructures and their structural transformation induced by high pressure. Fullerene nano/microcrystals with controllable size, morphology and structure have been synthesized through the self-assembly of fullerene molecules by a solvent-assisted method. By virtue of high pressure, the structures, components, and intermolecular interactions of the assemblied fullerene nano/microcrystals can be finely tuned, thereby modifying the optical and electronic properties of the nanostructures. Several examples on high pressure induced novel structural phase transition in typical fullerene nanocrystals with C60 or C70 cage serving as build- ing blocks are presented, including high pressure induced amorphization of the nanocrystals and their bulk moduli, high pressure and high temperature (HPHT) induced polymerization in C60 nanocrystals, pressure tuned reversible polymeriza- tion in ferrocene-doped C60/C70 single crystal, as well as unique long-range ordered crystal with amorphous nanoclusters serving as building blocks in solvated C60 crystals, which brings new physical insight into the understanding of order and disorder concept and new approaches to the design of superhard carbon materials. The nanosize and morphology effects on the transformations of fullerene nanocrystals have also been discussed. These results provide the foundation for the fabrication of pre-designed and controllable geometries, which is critical in fullerenes and relevant materials for designing nanometer-scale electronic, optical, and other devices. 相似文献
6.
单壁碳纳米管在不同材质基片银膜上的表面增强拉曼光谱 总被引:2,自引:0,他引:2
在玻璃、白宝石和石英基片上,利用化学沉积法和溶胶法制备了纳米结构活性银膜,系统地研究了两种不同方法制备的单壁碳纳米管(SWNT)的表面增强拉曼光谱(SERS)的G带和D带.同一样品的G带,在不同基片上的峰移量不同,在白宝石基片上移动更大,峰强更高,可以更敏感地反映SERS效应.D带的峰形随基片不同而改变.金属性管的含量较高的样品,其D带光谱的峰移较半导体性管含量较高的样品更显著,表明金属性碳纳米管与SERS活性银膜的界面相互作用更强. 相似文献
7.
通过溶剂挥发法获得了准一维C70纳米/亚微米棒状晶体,直径为~500nm, 长度为~10μm,呈六方密堆(hcp)结构. 利用金刚石对顶砧(DAC)高压装置,采用同步辐射能量色散X光能量色散衍射方法(EDXD)和高压拉曼光谱,研究了压力对C70纳米/亚微米棒结构的影响, 实验中最高压力为26.1GPa. 结果表明, 在准静水压条件下,在23.3—26.1GPa压力范围内, hcp结构的C70纳米/亚微米棒发生了由hcp结构向非晶化的相变,相变压力比体材料高约5GPa, 该相变是不可逆相变, 而且该相变是由于C70在高压下笼状结构被破坏所导致的. 相似文献
8.
采用气相扩散方法将C60分子填充到单壁碳纳米管(SWNTs)中,制备出高填充比率的豆荚形纳米材料C60@SWNT,又称为peapod.用金刚石对顶砧(DAC)装置获得高压,在高压下同时利用紫外激光处理样品,通过激光和压力的共同作用研究了C60分子在碳管内的聚合相变.在21.5 Gpa高压下,同时紫外激光(325 nm)照射30 min后,拉曼光谱表明C60分子在碳管内发生了聚合,形成一维链状O相聚合结构,且该相变是不可逆的.紫外激光的引入使样品发生O相聚合所需的压力值低于仅由压力诱导的聚合压力. 相似文献
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10.
使用第一原理密度泛函计算方法,我们研究了(5,5)有限长单壁碳纳米管(FSWNT)在气相条件下,结构的变化对振动模式(红外强度和拉曼活性)的影响. 我们得到了与无限长单壁碳纳米管(SWNT)有差异的拉曼频谱,发现了A1g, E1g 和 E2g的不同频移特征,并对其原因进行了解释. 当结构压缩到1.5 时,我们得到了一个双管的FSWNT结构,它也具有一个呼吸模(409.26 cm-1),而释放“压力”之后,FSWNT不同于SWNT之处在于其不能恢复到理想的D5d对称性结构,我们得到了一个新的具有C2h对称性的稳定的两端半封闭的FSWNT,其也具有一个明确的呼吸模(365.01 cm-1). 并且,我们发现了稳定的D5d和C2h对称性结构的不同的电子布居特征. 相似文献