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1.
BN纳米管——一种新型的纳米材料   总被引:1,自引:0,他引:1  
邢光建  陈光华 《物理》2002,31(3):151-154
文章综述了BN纳米管的最新进展,介绍了BN纳米管的结构和制备技术发展情况,包括电弧放电,电弧熔融,激光烧蚀,机械球磨,碳纳米管取代反应答经学反应法,探讨了BN纳米管的机械和电学性质,并展望了BN纳米管的应用前景,提出了BN纳米管的发展方向。  相似文献   

2.
单壁碳纳米管轴向压缩变形的研究   总被引:4,自引:0,他引:4       下载免费PDF全文
王宇  王秀喜  倪向贵  吴恒安 《物理学报》2003,52(12):3120-3124
采用Tersoff-Brenner势函数描述碳纳米管中碳原子间的相互作用,通过分子动力学方法对不同螺旋型的单壁碳纳米管的轴向压缩变形行为进行了研究.研究发现单臂碳纳米管的杨氏模量低于锯齿形碳纳米管,根据微观结构特征的差异对这一结果进行了分析.同时从能量和结构变化两方面对碳纳米管受压失稳进行了分析,揭示出碳纳米管失稳的微观特征. 关键词: 纳米管 分子动力学 杨氏模量 屈曲  相似文献   

3.
碳纳米管自发现以来,由于其独特的结构和奇特的物理,化学和力学特性以及其潜在的应用前景而倍受人们的关注。本文介绍近年来这一前沿研究领域所取得的部分重要研究进展,并讨论碳纳米管的几种应用前景。  相似文献   

4.
碳纳米管电子学的研究与进展   总被引:1,自引:0,他引:1  
杨铮  施毅  顾书林  沈波  张荣  郑有炓 《物理》2002,31(10):624-628
简单回顾了碳纳米管的电学性质以及各种基于碳纳米管的电子器伯,最新发现的碳纳米管的双极型性质也作了简单报道,着重讨论了由碳纳米管构成的逻辑电路,阐明了碳纳米管电子学发展过程将遇到的困难和挑战,了碳纳米管电子学的未来和应用前景。  相似文献   

5.
碳、碳氮和硼碳氮纳米管场发射性能的比较研究   总被引:4,自引:0,他引:4       下载免费PDF全文
李强  梁二军 《物理学报》2005,54(12):5931-5936
采用高温热解法在860℃分别制备出了碳、碳氮和硼碳氮纳米管,提纯后利用丝网印刷工艺分别将它们制备成薄膜,并测试了它们的场发射性能.结果表明:碳纳米管、碳氮纳米管和硼碳氮纳米管薄膜的开启电场分别为2.22,1.1和4.4V/μm,当电场增加到5.7V/μm时,它们的电流密度分别达到1400,3000μA/cm2和小于50μA/cm2.碳和碳氮纳米管薄膜的场增强因子分别为10062和11521.可见,碳氮纳米管的场发射性能优于碳纳米管,而硼碳氮纳米管的场发射性能比前两者要差.解释了这三种纳米管场发射性能差别的原因. 关键词: 碳纳米管 碳氮纳米管 硼碳氮纳米管 场发射  相似文献   

6.
碳纳米管晶格振动模及拉曼光谱的研究进展   总被引:7,自引:0,他引:7  
本文介绍了碳纳米管的结构特征和晶格振动模的理论研究 ,综述了不同方法生长的多壁碳纳米管和单壁碳纳米管拉曼光谱的研究进展。另外 ,还简单描述了单壁碳纳米管的应用前景  相似文献   

7.
周震  赵纪军 《物理学进展》2007,27(1):92-108
碳纳米管较低的碳原子密度、管径和管间的空隙可以为锂离子提供大量的嵌入空间,从而拥有更高的储锂能力。本文结合实验与理论研究的最新成果,综述了这一领域的主要进展和前景。实验上,对单壁碳纳米管进行适当处理,可以将锂存储量提高到常规石墨材料的2~3倍。根据密度泛函理论计算,锂在不同碳纳米管束中的最高理论嵌入量可以达到Li0.5C。嵌入后锂和碳纳米管之间发生了完全的电荷转移,碳纳米管的Fermi能级上移到导带中,所有碳纳米管都转变为金属。纳米管自身的电子结构对锂的吸附是至关重要的,缺电子体系更有利于锂的吸附。锂在B掺杂的复合管如BC3纳米管中有很大的吸附能。锂穿透纳米管壁从管壁外进入纳米管内的能垒,随着纳米管壁拓扑缺陷结构的尺寸变大而显著降低,B在纳米管壁的存在会进一步降低锂穿越纳米管壁的能垒。同时B的掺杂会降低相同拓扑缺陷的生成能,导致在BC3纳米管中出现更多的拓扑缺陷,从而有利于锂离子的扩散。实验与理论计算的结合可望加深对锂离子在纳米管材料中嵌入过程的理解,指导设计具有更高储锂性能的新材料。  相似文献   

8.
周震  赵纪军 《物理学进展》2011,27(1):92-108
碳纳米管较低的碳原子密度、管径和管间的空隙可以为锂离子提供大量的嵌入空间,从而拥有更高的储锂能力。本文结合实验与理论研究的最新成果,综述了这一领域的主要进展和前景。实验上,对单壁碳纳米管进行适当处理,可以将锂存储量提高到常规石墨材料的2~3倍。根据密度泛函理论计算,锂在不同碳纳米管束中的最高理论嵌入量可以达到Li0.5C。嵌入后锂和碳纳米管之间发生了完全的电荷转移,碳纳米管的Fermi能级上移到导带中,所有碳纳米管都转变为金属。纳米管自身的电子结构对锂的吸附是至关重要的,缺电子体系更有利于锂的吸附。锂在B掺杂的复合管如BC3纳米管中有很大的吸附能。锂穿透纳米管壁从管壁外进入纳米管内的能垒,随着纳米管壁拓扑缺陷结构的尺寸变大而显著降低,B在纳米管壁的存在会进一步降低锂穿越纳米管壁的能垒。同时B的掺杂会降低相同拓扑缺陷的生成能,导致在BC3纳米管中出现更多的拓扑缺陷,从而有利于锂离子的扩散。实验与理论计算的结合可望加深对锂离子在纳米管材料中嵌入过程的理解,指导设计具有更高储锂性能的新材料。  相似文献   

9.
聚苯胺-碳纳米管复合体的制备及其光响应   总被引:11,自引:0,他引:11       下载免费PDF全文
纳米尺寸导电材料对功能分子材料及分子器件的作用越来越显得重要.采用原位乳液聚合法制备聚苯胺 碳纳米管复合体,SEM和TEM照片显示复合管的直径为60—70nm,聚苯胺的包裹层厚度约25—30nm.x射线衍射及热分析表明纳米复合管的结晶性能增强,热稳定性得到提高.光电响应试验表明复合管的光吸收增强,光电流增大,说明聚苯胺 碳纳米复合管薄膜受光照射后发生了光诱导电荷分离现象. 关键词: 聚苯胺 碳纳米管 复合纳米管 光电流  相似文献   

10.
采用Tersoff势测试和研究了反向非平衡分子动力学中的Müller-Plathe法和Jund法在一维纳米管热传导中的应用.在相同的模拟步数中,Müller-Plathe法可以得到很好的结果,热导率在交换频率大于50时对参数的选择并不敏感.然而,Jund法并不能得到良好的线性温度梯度,其热导率在一定程度上依赖于选择的热流大小.在此基础上,运用Müller-Plathe法进一步研究了碳纳米管和碳化硅纳米管的长度、直径和温度对热导率的影响.结果表明,无论是碳纳米管还是碳化硅纳米管,其长度、直径和温度对热导率的影响是一致的.只要长度增加,纳米管的热导率相应增大,但增长速率不断降低.直径对热导率的影响很大程度上还取决于温度,在高温时,直径对热导率几乎没有影响.除此之外,纳米管的热导率随着温度的增加总体上也是不断降低的,但峰值现象的出现还受纳米管长度的影响.  相似文献   

11.
Peter J.F. Harris 《哲学杂志》2013,93(18):2355-2363
The formation of novel structures by the passage of an electric current through graphite is described. These structures apparently consist of hollow three-dimensional graphitic shells bounded by curved and faceted planes, typically made up of two graphene layers. The curved structures were frequently decorated with nano-scale carbon particles, or short nanotubes. In some cases, nanotubes were found to be seamlessly connected to the thin shells, indicating that the formation of the shells and the nanotubes is intimately connected. Small nanotubes or nanoparticles were also sometimes found encapsulated inside the hollow structures, while fullerene-like particles were often seen attached to the outside surfaces. With their high surface areas and structural perfection, the new carbon structures may have applications as anodes of lithium ion batteries or as components of composite materials.  相似文献   

12.
吴群  王玥  吴昱明  庄蕾蕾  李乐伟  桂太龙 《中国物理 B》2010,19(6):67801-067801
This paper investigates the radiation characteristics of metal single-walled zig-zag carbon nanotubes as a dipole antenna at terahertz wave range. The current distribution, input impedance and mutual impedance are calculated for various geometrical parameters of vertically-aligned carbon nanotubes. The numerical results demonstrate the properties of the antenna depending strongly on the geometrical parameters such as the radius, the lengths of carbon nantobues, and the spacing between nanotubes. It is found that the zig-zag carbon nanotubes exhibit very high input impedance and the mutual impedances for antenna array applications. These unique high impedance properties are different from the conventional metal thin wire antenna. The far-field patterns and gain of antenna array are also calculated. The maximum gain of array of 100-element array is up to 20.0~dB, which is larger than the gain of 0.598~dB of single dipole antenna at distance d = 0.5\lambda .  相似文献   

13.
The invention of carbon and its allotropes have transformed the electronic and optoelectronic industry due to their encouraging properties in a large spectrum of applications. The interesting characteristic of carbon is its ability to form many allotropes due to its valency. In recent decades, various allotropes and forms of carbon have been invented, including fullerenes, carbon nanotubes (CNTs), and graphene (GR). Since the inception of nanotechnology, carbon allotropes-based nanocomposites have become a leading sector of research and advancement due to their unique bonding properties. Fullerenes and CNTs-based polymer nanocomposites have attracted significant research interest due to their vast applications in every sphere of science and technology. Current research impetus reveals that carbon and its allotropes have revolutionized the industry and academia due to their fascinated properties. Recent advances in various aspects of graphene, CNTs, graphene nanoribbons, fullerenes, carbon encapsulates, and their nanocomposites with polymeric materials and their different applications are reported in this review article. Also, current status and future prospects of graphene-based polymer nanocomposites are presented in common along with proper citations extracted from the scientific literature. Moreover, this article is a unique collection of vital information about GR, CNTs, fullerenes, and graphene-based polymer nanocomposites in a single platform.  相似文献   

14.
高纯度和高产率的制备碳纳米管是碳纳米管研究的一个重点。目前制备碳纳米管的方法有电弧法、激光蒸发法、化学气相沉积法(又称CVD法)和模板法等。本文主要介绍采用PECVD化学气相沉积法制备碳纳米管,并对该种方法制备碳纳米管进行了系统的研究和探讨。  相似文献   

15.
赵华波  李震  李睿  张朝晖  张岩  刘宇  李彦 《物理学报》2009,58(12):8473-8477
利用导电型原子力显微镜对大范围碳纳米管(CNT)网络的导电性能进行成像观察.研究发现:在几十微米的成像范围内,每根CNT本身的电阻远小于CNT之间的接触电阻,以致于在电压偏置的网络中不同的CNT呈现电位不同的等位体;CNT的导电性能虽不因与其他CNT的交叠接触而改变,但是如果缠绕成束,则半导体性CNT趋于呈现金属性CNT的导电特征. 关键词: 导电型原子力显微镜 碳纳米管网络 碳管纳米电导  相似文献   

16.
We have investigated the morphology and microstructure of carbon nanotubes and nanoparticles in cathode deposits prepared by self-sustained arc discharge. Scanning electron microscopy images indicate that there are two regions exhibiting different morphologies on the top surface of the cathode deposits. In the central region, there is a triangular pattern of spots with a diameter up to 100μm, which consists of carbon nanotubes and nanoparticles. In the fringe region, carbon nanotubes and nanoparticles are distributed randomly. In addition, carbon nanotubes in the central region have a larger inner diameter, compared with those in the fringe region. The outer diameter distribution of tubes in the central region is narrower than that of tubes in the fringe region, while the former has a smaller peak value than the latter. For the nanoparticles, they exhibit a different behaviour from the tubes existing in the same region. The difference between the microstructure of tubes or particles in the two regions is attributed to the different temperatures and temperature gradients during their formation.  相似文献   

17.
李瑞  胡元中  王慧 《物理学报》2011,60(1):16106-016106
本文采用分子动力学模拟方法研究了Si表面间单壁水平碳纳米管束SWCNT (10,10)的变形和摩擦特性.系统在弛豫平衡后,首先对碳纳米管束施加压力至碳纳米管或Si表面结构破坏.之后在无压力和高压力两种情况下使上表面沿水平方向做剪切运动以研究碳纳米管束的摩擦特性.结果表明,由于碳纳米管的柔韧性,碳纳米管束在加载过程中出现明显变形,但直至3.8 GPa高压下并无结构破坏.系统无压力时SWCNT (10,10)在原地轻微随机滚动,压力为3.8 GPa时,碳纳米管束出现了整体的轻微滑动,同时伴随无规律的轻微滚动, 关键词: 碳纳米管束 摩擦 分子动力学模拟  相似文献   

18.
单壁碳纳米管杂化轨道计算   总被引:5,自引:0,他引:5       下载免费PDF全文
根据轨道杂化理论以及碳纳米管的几何结构,计算了(n,0),(n,n)和(n,m)三种单壁碳纳米管的杂化轨道,给出了杂化轨道s轨道成分和p轨道成分的解析式.对于管径较小的纳米管,锯齿型(n<40),扶手椅型(n<20),手性型(n<30,m相似文献   

19.
王磊  张忠强  张洪武 《物理学报》2008,57(11):7069-7077
在单壁碳纳米管电浸润现象原子模拟的基础上,对双壁碳纳米管的电浸润现象进行了计算机模拟.运用经典分子动力学方法结合一个宏观的电毛细管模型模拟了双壁碳纳米管在水银中的电浸润过程,对不同内管尺寸情况下的浸润现象作了研究和比较.计算结果表明双壁碳管和单壁碳管的电浸润过程存在很大的不同,双壁碳管的内管在电浸润过程中起到重要的作用:当改变双壁碳管中内管的尺寸时,浸润现象会产生很大的改变. 关键词: 双壁碳纳米管 电浸润 分子动力学  相似文献   

20.
Through floating catalyst chemical vapour deposition(CVD) method,well-aligned isolated single-walled carbon nanotubes (SWCNTs) and their bundles were deposited on the metal electrodes patterned on the SiO2/Si surface under ac electric fields at relatively low temperature(280℃). It was indicated that SWCNTs were effectively aligned under ac electric fields after they had just grown in the furnace.The time for a SWCNT to be aligned in the electric field and the effect of gas flow were estimated. Polarized Raman scattering was performed to characterize the aligned structure of SWCNTs. This method would be very useful for the controlled fabrication and preparation of SWCNTs in practical applications.  相似文献   

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