首页> 外文学位 >Traveling-waves in DC-biased metallic carbon nanotubes: Theoretical investigation of amplification and fabrication of characterization fixture .
【24h】

Traveling-waves in DC-biased metallic carbon nanotubes: Theoretical investigation of amplification and fabrication of characterization fixture .

机译:直流偏置金属碳纳米管中的行波:表征夹具的放大和制备的理论研究。

获取原文
获取原文并翻译 | 示例

摘要

Radio-frequency (RF) generation and amplification is at the heart of telecommunication, satellite and optoelectronics applications. The electronics industry is in constant search for RF amplifiers that are smaller, more efficient, and operating at higher frequencies. Nanomaterials with unique properties promise to fulfill these characteristics while bridging the gap between vacuum-based and solid-state amplifiers. In this thesis, we specifically investigate the capability of carbon nanotubes (CNTs) in amplification of traveling-waves at RF frequencies. Using theoretical means, we show that such amplification is indeed a possibility. We also design and fabricate the characterization fixture needed for measurements and testing the theory.;Over the last two decades, CNTs have proved that they possess remarkable electrical properties. Two of these properties incite the following study. First, CNTs possess a large electron drift velocity due to their long mean free path at room temperature. Furthermore, electromagnetic surface-wave propagation along a CNT acquires a large slow-wave factor due to the smallness of the radius and the infinitesimal wall thickness. The drift and phase velocities are calculated to be on the same order of magnitude, thereby immensely motivating this study : such synchronization between the electrons and the RF field is exactly the physical mechanism used in traveling-wave tubes (TWTs) to induce amplification.;In general, the theoretical problem is to investigate the outcome of applying simultaneous DC and RF fields across a metallic-CNT. For this purpose, the CNT current density is first calculated through a semi-classical transport problem. Then, through coupling with the electromagnetic problem, an eigenmode solution is reached. Finally, RF traveling-wave amplification is found above a certain threshold DC field.;Particularly, from the particle's transport perspective, we use the Boltzmann transport equation (BTE) to calculate the distribution of the charge carriers under DC and AC fields. Afterwards, the Boltzmann AC current density is found with respect to the applied DC field. Negative differential conductivity (NDC) is found under moderate fields. By approximating the electronic dispersion of CNTs as a linear function, we find analytical solutions for the distribution and current density that agree reasonably well with the full-band numerical solution of the differential equations.;From the electromagnetic wave perspective, we use Maxwell's equations to find the solution for surface-wave propagation along a hollow conductor which is the CNT. Using the surface boundary conditions, we reach a relation for the Maxwell current density. By equating the currents calculated through the transport and electromagnetic aspects at all points in space-time, we find a determinantal equation whose solution is the electromagnetic dispersion.;In the absence of a DC field, the immense slow-wave factor in CNTs is attributed largely to the geometry of the problem. On the other hand, the RF propagation is found to be largely modulated by the application and subsequent increase of a DC field.;Assuming negligible spatial dispersion, an amplification was found beyond a threshold value of 3 x 105 V/m, as signalled by a positive attenuation factor. At such fields, the amplification response is explained in our model through Bloch-type reflections at the Brillouin zone (BZ) edges, instead of the expected TWT-like behavior.;However, preliminary calculations that included the spatial dispersion lead to the appearance of an amplified mode at a lower field of 10 4 V/m. Interestingly, the phase and drift velocities are matched at this field magnitude, which suggests a possibility of a TWT-like amplification. However crude, these results point to the importance of the previously neglected non-local effects, which are worthy of a more rigorous calculation that makes use of complex plane analysis techniques.;Due to technical shortcomings, the experimental aim of the work was limited to the design and fabrication of the RF characterization fixture which could later be used to investigate the problem experimentally. The coplanar waveguide (CPW) was the planar waveguide of choice thanks to its versatility and high-frequency capabilities. The CPW signal trace was tapered and a gap opening allowed for CNTs, ideally one, to be aligned for measurements. The CNTs were deposited on the substrates using spin-coating as a first step. Then, using the atomic force microscope (AFM), the deposition was refined to the desired concentration and alignment. Afterwards, the CPW electrodes were patterned using standard optical lithography/lift-off. After this final step, alignment across the CPW gaps was probed using the scanning electron microscope (SEM). As a result, we found numerous CPWs contacted by a single or multiple CNTs
机译:射频(RF)的产生和放大是电信,卫星和光电应用的核心。电子行业一直在寻找体积更小,效率更高且工作频率更高的RF放大器。具有独特性能的纳米材料有望满足这些特性,同时缩小基于真空的放大器与固态放大器之间的差距。在本文中,我们专门研究了碳纳米管(CNTs)在RF频率下行波放大的能力。使用理论方法,我们证明了这种放大确实是可能的。我们还设计和制造了用于测量和测试理论的表征夹具。在过去的二十年中,CNT已证明它们具有出色的电性能。这些属性中的两个引发了以下研究。首先,由于CNT在室温下具有较长的平均自由程,因此具有较大的电子漂移速度。此外,由于半径小且壁厚无穷小,因此沿CNT传播的电磁表面波会获得较大的慢波因子。计算得出的漂移和相速度处于相同的数量级,从而极大地推动了这项研究:电子与RF场之间的这种同步正是行波管(TWT)用来引起放大的物理机制。通常,理论问题是研究在金属CNT上同时施加DC和RF场的结果。为此,首先通过半经典传输问题计算CNT电流密度。然后,通过与电磁问题耦合,获得本征模解。最后,在一定的阈值DC场以上发现RF行波放大。特别是,从粒子的传输角度,我们使用Boltzmann传输方程(BTE)来计算DC和AC场下载流子的分布。之后,相对于所施加的直流场,找到了玻尔兹曼交流电流密度。在中等电场下发现负电导率(NDC)。通过将碳纳米管的电子色散近似为线性函数,我们找到了分布和电流密度的解析解,这些解析解与微分方程的全频带数值解相当吻合;从电磁波的角度来看,我们使用麦克斯韦方程来找到表面波沿着中空导体CNT传播的解决方案。使用表面边界条件,我们得出麦克斯韦电流密度的关系。通过将在时空所有点上通过输运和电磁方面计算出的电流相等,我们找到了一个行列式方程,其解是电磁色散。在没有直流磁场的情况下,碳纳米管中的巨大慢波因子被归因于在很大程度上取决于问题的几何形状。另一方面,发现RF传播在很大程度上受应用和随后DC场增加的调制。;假设空间色散可忽略不计,发现放大值超过3 x 105 V / m的阈值,这表明正衰减系数。在这样的场上,我们的模型通过布里渊区(BZ)边缘的Bloch型反射而不是预期的类似TWT的行为来解释放大响应;然而,包括空间色散在内的初步计算导致出现了在10 4 V / m的较低场的放大模式。有趣的是,相位和漂移速度在该场大小下匹配,这表明存在类似TWT放大的可能性。然而,粗略的说来,这些结果指出了以前被忽略的非局部效应的重要性,这值得利用复杂的平面分析技术进行更严格的计算。由于技术上的缺陷,这项工作的实验目的仅限于射频表征夹具的设计和制造,以后可用于通过实验研究该问题。共面波导(CPW)由于其多功能性和高频性能而成为首选的平面波导。 CPW信号走线逐渐变细,并且允许将CNT(理想的一种)的缝隙开口对齐以进行测量。第一步,使用旋涂将CNT沉积在基板上。然后,使用原子力显微镜(AFM),将沉积物精炼至所需浓度和排列。之后,使用标准的光刻/剥离图案化CPW电极。在此最后步骤之后,使用扫描电子显微镜(SEM)探测CPW间隙的对齐情况。结果,我们发现单个或多个CNT接触了许多CPW。

著录项

  • 作者

    Dagher, Milad.;

  • 作者单位

    Ecole Polytechnique, Montreal (Canada).;

  • 授予单位 Ecole Polytechnique, Montreal (Canada).;
  • 学科 Engineering Electronics and Electrical.;Physics Electricity and Magnetism.;Physics Condensed Matter.
  • 学位 M.Sc.A.
  • 年度 2012
  • 页码 85 p.
  • 总页数 85
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号