共查询到19条相似文献,搜索用时 125 毫秒
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在电弧放电方法制备碳纳米管中 ,通过用碳纳米管填充阳极进行放电实验 ,成功地得到了小直径单层碳纳米管 .同时在多层管的最内层得到了直径 0 5nm的碳纳米管 .这个结果表明直径小于C60 (直径 0 7nm)的碳纳米管是存在的 . 相似文献
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利用介质阻挡放电等离子体化学气相沉积技术,在蒸镀有25nm Ni催化剂层的Si基片上,以CH4和H2作为反应气体,在973K下制备了碳纳米管,并研究了微量水的引入对碳纳米管形貌的影响.场发射扫描电子显微镜结果表明,不加水时,制备出的碳纳米管直径不均匀,分布在40—90nm之间,呈链节状的结构;加入少量水时,制备出的碳纳米管直径比较均匀,集中在70nm左右,表面为瘤状结构;当水的流量进一步增加时,得到的碳纳米管表面光滑,出现了枝状结构.原位测量了加水前后等离子体区的发射光谱,分析了微量水的引入对于碳纳米管形貌变化的影响机理.
关键词:
碳纳米管
介质阻挡放电
水
发射光谱 相似文献
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多壁碳纳米管的拉曼散射 总被引:4,自引:1,他引:3
本文报导了用直流碳弧放电方法制备的多层碳纳米管的拉曼光谱。和HOPG相比,由于碳纳米管的量子尺寸效应和碳纳米管直径的分布,在纯化和未纯化的碳纳米管中均存在E2g模的软化,其红移范围分布在2~13cm 1范围内。 相似文献
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以Y/Ni为催化剂制备的单壁碳纳米管的拉曼光谱研究 总被引:1,自引:0,他引:1
采用电弧放电法以Y/Ni为催化制备了单壁碳纳米管(SWNTs),对样品进行了扫描电镜、透射电镜和拉曼光谱的研究。所制备的样品中单壁碳纳米管的含量较高。对单壁碳纳米管的共振拉曼散射增强效应进行了观察,随激光波长的不同,单壁碳纳米管的拉曼光谱也随之变化,尤其是低频区径向呼吸模的变化比较明显。利用布里渊区折叠法计算了单壁碳纳米管的电子态密度曲线,根据SWNTs电子态密度尖峰之间的能量差、管子的直径和呼吸模频率建立了一个图表,并对SWNTs的呼吸模进行了归属。分析结果表明:样品中单壁碳纳米管的直径分布在0.79-1.76nm范围,金属管和半导体管均存在,并且直径在1.45nm附近的碳管居多。 相似文献
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基于碳纳米管粗产品中无定形碳和不同直径碳纳米管对氧的反应活性的差异 ,通过差热 -热重 (TG DTA)方法 ,结合透射电镜 (TEM)和X射线衍射 (XRD)的测试结果 ,研究了合成温度对以乙炔气体为碳源 ,用CVD法制备碳纳米管的石墨化程度、碳纳米管直径以及直径分布的影响 .结果表明 :反应中 ,由于催化剂Co/SiO2中活性组分 (Co)微晶随合成温度的升高而增大 ,导致所制备的碳纳米管的直径增大 ,从 2 0~ 30nm (6 5 0℃ )增加到 30~ 5 0nm (75 0℃ ) .碳纳米管的石墨化程度随着反应温度的升高而增加 .XRD实验结果还表明 ,当合成温度从 6 5 0℃增加到 85 0℃时 ,2θ值从 2 5 .8°增加到 2 6 .8°,(0 0 2 )晶面的层间距从 3.45 减小到 3.32 ,即随着合成温度的升高 ,碳纳米管 (0 0 2 )晶面的层间距减小 .通过DTA放热峰的峰温和半峰宽的分析得出 ,无定形碳的放热峰峰温Tp<380℃ ,其含量随着温度的升高而减小 .碳纳米管的DTA放热峰的峰温Tp 随着碳纳米管的直径和石墨化的程度的增加而升高 ,半峰宽随着碳纳米管的直径的分布范围增大而增宽 .低温 (6 5 0℃ )有利于生成直径小且均匀的多层碳纳米管 (2 0~ 30nm) ,而高温 (大于 75 0℃ )则有利于生成直径大的多层碳纳米管 (大于 30~5 0nm) . 相似文献
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提出了透射电子显微镜(TEM)纳米云纹法的新技术,首次将该方法用于单根单壁碳纳米管的残余变形测量。纳米云纹由计算机显示器扫描线与碳纳米管束TEM图像干涉而成。该方法具有纳米级空间分辨率,可直接测量碳纳米管的力学性能。对TEM纳米云纹法的原理进行了详细的阐述,并利用不同管径的单壁碳管束产生了云纹。对直径为7.5nm的弯曲碳管束的残余变形进行测量,直接得到了其中一根直径为1.0nm的单壁碳管的残余变形场。实验结果证明了该方法的可行性。该方法为纳米尺度的碳管力学性能测量提供了新途径。 相似文献
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用微米级LaNi5合金粉末为催化剂, 以乙炔为原料, 采用化学气相沉积(CVD)法合成了多壁碳纳米管. 在100~290 K温度下测量了41 μm≤d≤150 μm粒径催化剂制备的不同直径分布的碳纳米管的电子自旋共振(ESR)谱,研究了测量温度、微米级催化剂粒径及制备过程的氢气氛对生成的碳纳米管的ESR谱线型、g因子、线宽的影响. 发现碳纳米管的g因子随其直径的增大而增大,分别为2.040 0(催化剂粒径41 μm≤d≤50 μm, 碳纳米管的直径分布为10 nm到20 nm)和2.089 8(催化剂粒径100 μm≤d≤150 μm,碳纳米管的直径分布为70 nm到120 nm). 发现小管径纳米管的ESR谱图有一个峰, 而大管径纳米管的ESR谱图有两个峰A和B, 且随测量温度的升高, 峰B强度增大. 相似文献
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The total carbo-mer of single-walled carbon nanotubes (C-SWCNTs) are constructed by inserting two sp carbon atoms into each C-C bond in pristine single-walled carbon nanotubes (SWCNTs). The geometric, mechanical and electronic properties for these novel structures are investigated by self-consistent-field crystal calculations. The calculated zigzag and chiral C-SWCNTs are all small gap semiconductors, whereas the metallic property is still kept in the armchair C-SWCNT. The calculated Young's moduli of C-SWCNTs are smaller than those of SWCNTs. Our calculations show that the zigzag C-SWCNTs have higher mobility than the corresponding SWCNTs. Moreover, the calculated mobility of the C-SWCNTs has a periodic change with the change of the tube diameters. 相似文献
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The impact of a nanosecond high-energy ion beam on the structure and morphology of multilayer carbon nanotubes and their ensembles is studied using transmission electron microscopy and scanning electron microscopy. It is shown that ion-beam irradiation leads to a decrease in the outer diameters of carbon nanotubes, which is related to the destruction of their outer layers. In addition, the secondary growth of carbon nanotubes with smaller diameters and the growth of bulblike formations, inside which structures with interplanar distances that are close to those of nanodiamond are fixed, are observed. 相似文献
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A theoretical model for the growth of single-wall carbon nanotubes produced by metal-catalyzed decomposition of hydrocarbons
and fullerenes is presented. The growth process is treated as a thermodynamic equilibrium between carbon in the gas phase
and carbon in the nanotube. The minimum possible nanotube diameters based on several published experimental conditions are
calculated by combining the free energy of the reaction with an equation derived from elastic theory. The model predicts the
possibility of generating nanotubes with extremely small diameters that are smaller than in the corresponding experiments.
Received: 18 July 2001 / Accepted: 19 November 2001 / Published online: 4 March 2002 相似文献
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Leyong Zeng Da Lei Weibiao Wang Jingqiu Liang Ning Yao 《Applied Surface Science》2008,254(6):1700-1704
Carbon nanosheets were synthesized by microwave plasma-enhanced chemical vapor deposition method on carbon nanotubes substrate which was treated by hydrogen plasma. The results showed that the diameters of carbon nanotubes first got thick and then “petal-like” carbon nanosheets were grown on the outer wall of carbon nanotubes. The diameters of carbon nanotubes without and with carbon nanosheets were 100-150 and 300-500 nm, respectively. Raman spectrum indicated the graphite structure of carbon nanotubes/carbon nanosheets. The hydrogen plasma treatment and reaction time greatly affected the growth and density of carbon nanosheets. Based on above results, carbon nanosheets/carbon nanotubes probably have important applications as cold cathode materials and electrode materials. 相似文献
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W.Q. Han L. Bourgeois Y. Bando K. Kurashima T. Sato 《Applied Physics A: Materials Science & Processing》2000,71(1):83-85
Nanotubes exhibiting a novel structure - boron nitride (BN) conical nanotubes whose walls consist of conical layers with their cone axis parallel to the tube axis, as opposed to ordinary nanotubes, composed of concentric cylindrical layers with their normal perpendicular to the tube axis - were synthesized simultaneously with BN nanotubes by using carbon nanotubes (CNTs) as templates. The diameters of the BN conical nanotubes are typically about 15 nm, which is similar to those of the starting CNTs. Apex angles and inner diameters of most BN conical nanotubes are about 40° and 1 nm, respectively. The lengths of the BN conical nanotubes range from 50 nm to up to several micrometers. 相似文献
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Jin-Xing Shi Toshiaki Natsuki Qing-Qing Ni 《Applied Physics A: Materials Science & Processing》2014,117(3):1103-1108
Radial buckling stresses of carbon nanotubes (CNTs) need to be studied in high-pressure resonance Raman scattering spectrum. In this work, the closed-form expression of the critical buckling stress of multi-walled carbon nanotubes (MWCNTs) under hydrostatic pressure is derived that can be conveniently employed. Using the derived formulae, the critical buckling stresses of single-walled carbon nanotubes and double-walled carbon nanotubes with different diameters are calculated. The results are in good agreement with other reported literatures. In addition, the critical buckling stresses of each layer of a quintuple-walled CNT in different buckling modes are predicted, showing that the buckling instability can occur not only in the outermost rolled layer, but also in other rolled layer of MWCNTs by considering different diameters and buckling modes. 相似文献
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Multiwall carbon nanotubes were synthesized on the FeCoCaO and FeMoCaO catalysts by RF-CCVD at 750 °C, 850 °C and 950 °C, using acetylene as the carbon source. Analytically, it was found that the nanotubes are well crystallized, with outside diameters ranging between 10 and 60 nm and a ratio of the outside to the inside diameters of 2 to 3. The nanotubes did not present amorphous carbon and their purity increased with the temperature of synthesis. A relatively large number of metallic nanoparticles of various dimensions and shapes encapsulated inside the nanotubes were observed by TEM in most of the nanotube samples. 相似文献
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I. V. Osipova N. G. Vnukova G. A. Glushchenko A. S. Krylov E. V. Tomashevich S. M. Zharkov G. N. Churilov 《Physics of the Solid State》2009,51(9):1972-1975
This paper presents the results of an investigation of nickel-containing carbon nanostructures prepared by plasma-chemical
synthesis in a carbon-helium plasma jet at atmospheric pressure with the arc fed by a high-frequency current. It is demonstrated
that, under these conditions, the conversion of graphite into a carbon condensate reaches 98 wt % and the contents of carbon
nanotubes and nickel in this condensate are 72 and 10 wt %, respectively. Sequential treatment with nitric and hydrochloric
acids has made it possible to extract purified carbon nanotubes and nickel nanoparticles coated with a carbon shell (approximately
50 nm thick) in which the nickel content is 4 wt %. Data are presented on the diameters of the prepared nanotubes and on the
state of carbon in the samples. 相似文献