TEM喇叭天线低频补偿实验研究

 通过对TEM喇叭天线低频补偿的实验,验证了低频补偿原理的正确性。低频补偿可以改善TEM喇叭天线的低频传输特性及低频辐射特性。当TEM喇叭天线与低频补偿回路形成电偶极子和磁偶极子满足匹配条件时,天线低频辐射的单向性将得到提高。当天线的低频补偿回路形成的磁偶极矩足够大时,低频补偿可增大天线主辐射方向的辐射,并改善天线低频辐射特性。     

电-磁振子组合型超宽带天线数值分析

 采用CST MICROWAVE STUDIO电磁场数值计算软件,对电-磁振子组合型超宽带（UWB）天线结构参数与天线性能之间的物理关系进行了分析。电磁组合型天线的物理结构包括三部分：天线的馈电系统、TEM喇叭辐射单元和电流环辐射单元。激励源采用高斯脉冲，边界为6层理想吸收边界（PML6）。仿真结果表明：组合天线的外导体屏蔽和电流环分别改善了不同频带内的端口参数；当电流环周长(105 cm)约等于天线尺寸(50 cm)的2倍时，天线的反射能量较小，端口参数曲线平坦；天线的物理尺寸决定其辐射带宽，尺寸越大，低频辐射特性越好。     

电-磁振子组合型小型化超宽带天线研究

 采用频域分析的方法，对电-磁振子组合型超宽带天线物理特性进行了研究，结果表明：天线中的电振子和磁振子在波的传输和辐射过程中起互补作用，扩展了小尺寸天线的工作频带，提高了天线的辐射效率。还给出了50cm天线的模拟和测量结果：电压驻波比小于3时，天线带宽大于10倍频程，模拟与测量结果基本吻合。     

组合振子天线实验研究

组合振子是超宽带天线研究的一个重要方向，因为这种天线从设计的一开始就考虑到了低频辐射能力的提高，并采用电偶极子和磁偶极子组合的方式，力图使得振子主辐射方向上的波阻抗与自由空间相匹配，从而保证辐射场为纯净的TEM波。     

利用光晶格自旋链中磁振子的激发模拟有限温度下光子的动力学 Casimir 效应

研究了在静磁场诱导的磁偶极-偶极相互作用和外部激光场诱导产生的偶极-偶极相互作用下光晶格自旋链中磁振子激发的动力学特征. 文中选取了蓝失谐光晶格, 提出了等效温度的概念, 并将系统中磁振子的激发过程与光学振动腔中光子的激发过程进行了类比. 研究表明, 通过选取适当的系统参数, 可以在磁振子系统中重现有限温度下光子的动力学Casimir效应. 关键词： 光晶格 偶极－偶极相互作用 磁振子 Casimir效应     

光偶极天线的远场方向性研究

用时域有限差分方法模拟了两种光偶极天线模型的场分布,研究了光偶极天线的远场辐射特性随其长度增加而变化的规律以及影响其远场方向性的因素,发现光偶极天线的远场方向性随其长度增加而变化的规律类似于经典对称振子天线的相应规律.但高阶局域表面等离激元模式的存在使得光偶极天线的远场辐射图更快地出现了旁瓣.这些发现对于提高光天线的性能具有重要意义. 关键词： 光偶极天线 局域表面等离激元 金纳米粒子 远场方向性     

TEM喇叭天线低频补偿实验

TEM喇叭天线因为其较宽的带宽及辐射相位中心的不变性，成为超宽带（UWB）最常用的天线。标准TEM喇叭由两块三角形平板组成，对于低频TEM喇叭天线相当于开端平板传输线，有许多低频能量反射回信号源，这将影响源的工作，在大功率的情况下会对源造成损害。在引入加载低频补偿回路后，可吸收这部分低频能量，并改善天线的低频传输特性及低频辐射特性。     

磁谐振和电谐振结构构成的左手材料设计

用磁谐振器和电谐振器组合构成左手材料是设计左手材料的一个重要方法.基于这一设计方法,提出了能够抑制双各向异性的磁谐振器和电谐振器设计原理,即单回路镜像对称设计原理和双(四)回路镜像对称设计原理.根据这两个设计原理,设计了具有双负特性(负介电常数和负磁导率)的新结构,并通过实验仿真验证了结构的双负特性,从而验证了两种设计原理的正确性.所提出的两个设计原理以及新结构对于设计新型左手材料具有重要的实际意义和指导意义. 关键词： 左手材料 单回路镜像对称 双回路镜像对称     

电-磁振子组合型宽带高功率微波辐射天线仿真与设计北大核心CSCD

为了满足宽带高功率微波辐射系统紧凑化的需求,设计了一个口径面尺寸为20cm×20cm 的电 磁振子组合型天线,采用三维全波电磁场仿真,得到该天线在0.3～1.7GHz 带宽内的驻波比小于3,且在此带宽内天线增益均大于2.仿真分析了该天线结构的尺寸、电流环长度以及天线开口角度对电 磁振子组合型天线阻抗带宽和增益的影响.在此基础上,给天线馈入峰值为226kV 的宽带信号,仿真得到天线的最大辐射因子为150kV,等效峰值功率为358.8 MW,辐射效率约70.6%.仿真结果表明：组合振子天线能够满足宽带高功率微波的辐射要求,同时满足辐射系统紧凑化和高辐射效率的要求.     

复合振子天线辐射特性的数值模拟

 讨论了由电单极子和磁振子组合而成的复合振子天线结构和工作原理,用时域有限差分方法模拟了天线的辐射特性,计算了天线从同轴线的馈电效率,对于单极脉冲和双极脉冲馈源,馈电效率分别为65%和81%。给出了天线的电压驻波比、辐射近场和远场、能量方向图等。模拟结果表明：在H面内辐射方向图是轴线对称的,其形状是心型;在E面内,方向图关于轴线不对称,辐射最大值方向向上偏离大约15°。这种天线具有宽带特性和较高的馈电效率,适合于超宽带电磁脉冲辐射的天线阵列的应用。     

光电导天线辐射阻抗特性模拟分析(英文)

针对连续太赫兹光电导天线辐射功率较低的缺点,利用有限积分方法对三种常用的光电导天线,包括偶极天线、蝶形天线和螺旋天线,进行数值模拟并分析比较其辐射阻抗特性.仿真结果表明,偶极天线的辐射阻抗与偶极长度、宽度、电极间隙以及传输线宽度有关,且在其谐振频率存在峰值阻抗,适用于特定频率的太赫兹波辐射.蝶形天线和螺旋天线在所研究的太赫兹波段具有近似稳定的辐射阻抗,广泛应用于宽带领域.对带有交叉电极的电极间隙进行计算,结果表明由交叉电极引入的附加电容降低了天线的高频阻抗.     

Wideband dipole antenna with inter-digital capacitor

A dipole antenna with wideband characteristics is presented. The proposed antenna consists of a dipole with periodic capacitive loading and a pair of coplanar striplines (CPSs) as an impedance transformer. By adding interlaced coupling lines at each section, periodic capacitive loading is realized. The periodic interlaced coupling lines divide each arm of the dipole into five sections, and currents are distributed on different sections at different frequencies, which is useful to achieve a wide impedance bandwidth. By parametric study using HFSS, the optimized parameters of this dipole antenna are obtained. In order to validate the simulation results, a prototype of the proposed dipole antenna is fabricated and tested. The results show that the proposed antenna can achieve a gain of 3.1 dB-5.1 dB and bandwidth of 51% for |S 11 | < 10 dB over the band of 3.9 GHz-6.6 GHz, indicating its good radiation performance and radiation efficiency.     

Characterization of the radiation from single-walled zig-zag carbon nanotubes at terahertz range

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 .     

A traveling-wave stripline dipole antenna on a substrate lens at terahertz frequency

In this paper, a study of a stripline dipole antenna on a substrate lens used as a photoconductive detector in a terahertz system is presented. The traveling-wave behavior of the stripline dipole and the influence of the substrate lens are investigated over a broad frequency range up to 5.0 THz. The numerical results show that the lens shape represented by the ratio of the extension length to the lens radius plays an important role in maximizing the antenna gain and radiation spectral bandwidth. The gain response exhibited an increased level of sensitivity to the lens shape as the lens size increased, and this is particularly important in optimizing large substrate lenses. Improvements in the gain level over the entire frequency range of interest were observed as the lens diameter increased. This study provides helpful guidelines in choosing and optimizing a substrate lens designed for a terahertz photoconductive antenna, which is particularly useful for specific applications requiring a miniaturized photoconductive antenna design.     

不同渐变方式的喇叭结构对电-磁振子组合型超宽带天线特性的影响

 电-磁振子组合型超宽带（UWB）天线的物理结构包括3部分：天线的馈电系统、TEM喇叭辐射单元和电流环辐射单元。采用CST MICROWAVE STUDIO电磁场数值计算软件,对该组合型天线的结构与端口S参数和时域辐射特性的关系进行了分析。仿真结果表明：当TEM喇叭辐射单元和电流环辐射单元由3段金属板构成时，天线的端口S参数较小，主轴辐射功率较大，方向性较好。     

时间延迟对偶极子光导天线空间功率合成影响分析

对偶极子光导天线空间功率合成中时间延迟的影响进行了分析。利用太赫兹时域光谱技术分别获取了34, 500, 1000 m偶极子光导天线的太赫兹时域光谱。采用数值模拟方法分析时间延迟对空间功率合成的影响。结果发现:在满足空间功率合成时域相干度60%的条件下,两个34, 500, 1000 m偶极子光导天线阵列的相对最大时间延迟分别为350.7, 467.6, 450.9 fs;三个34, 500, 1000 m偶极子光导天线阵列的相对最大时间延迟分别为191.1, 250.5, 267.2 fs;四个34, 500, 1000 m偶极子光导天线阵列的相对最大时间延迟分别为167, 200.4, 217.1 fs。试验结果表明,空间功率合成数值模拟仿真能为偶极子光导天线阵列的物理实验提供重要依据。     

基于宽波束磁电偶极子天线的宽角扫描线性相控阵列

设计并加工了两款基于宽波束磁电偶极子天线单元的宽角扫描线性阵列.首先,通过加载磁偶极子的方法拓展了天线单元的3-dB波束宽度.然后,基于该宽波束天线单元设计了两款具有良好宽角扫描特性的一维阵列天线.实测结果表明,天线单元的E面方向图3-dB波束宽度在9GHz—12 GHz均大于107°,H面方向图3-dB波束宽度在7GHz—12 GHz均大于178°.E面阵列中心单元的有源驻波比在9GHz—13 GHz小于2,相对阻抗带宽为36.36%.H面阵列中心单元的有源驻波比在9.6GHz—12.6 GHz小于2.5,相对阻抗带宽为27.03%.E面阵列在9GHz—12 GHz可实现±70°的有效宽角扫描.H面阵列在9GHz—GHz可实现±90°的有效宽角扫描.与传统的扫描阵列相比,设计的阵列可实现有效宽带宽角扫描,在X波段相控阵雷达方面具有广阔的应用前景.     

Integration of microbolometers with infrared microstrip antennas

We report on various integration schemes of infrared microbolometers with microstrip antennas. The first integration design consists of two gold (Au) rectangular microstrip patches coupled along the radiating edges by a narrow niobium (Nb) strip. Devices using silicon oxide are compared to devices using amorphous silicon as antenna substrate. An extension of the twin-patch detector design is the microstrip dipole antenna-coupled microbolometer. Two ways of connecting the device to the contact pads via narrow dc leads are presented and compared. The contribution of the dc leads to the detector response is eliminated by directly connecting the dipole to the contact pads. The thermal isolation of the microbolometer from the silicon wafer is improved by incorporating air into the antenna dielectric substrate. This leads to higher detector responsivity and shifts the resonance towards longer antennas. The implementation of a bridge microstrip dipole antenna structure is also discussed.