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。     

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.     

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。     

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。     

小型L波段高功率微波辐射场测量系统接收天线

借鉴电-磁振子组合型天线结构,设计了一种基于同轴传输结构的小型L波段高功率微波(HPM)辐射场测量系统接收天线,解决了L波段传统波导型测量系统中接收天线体积大、使用不便的问题。通过仿真研究分析了天线结构尺寸与天线增益、驻波和方向图等特性参数之间的关系,优化设计了用于L波段HPM辐射场测量的接收天线结构,并对加工的天线实物进行了测试。结果表明:当天线口面尺寸与长度相等时,其边长与工作的中心频率对应波长存在着两倍的关系;选择边长为100mm可满足在1.2~1.8GHz频段内,天线驻波系数小于1.5,增益从2.8dB单调增大至6.1dB,方向图主瓣宽度大于70°,辐射主轴与天线几何主轴基本一致。     

低温下二维绝缘铁磁体的磁振子软化

在二维正方绝缘铁磁系统基础上建立了一个磁振子-声子相互作用模型.利用格林函数方法研 究了磁振子-声子相互作用下的二维绝缘铁磁体的磁振子谱, 计算了布里渊区的主要对称点 线上的磁振子色散曲线.发现在布里渊区边界区域磁振子谱的软化和磁振子谱线增宽最明显. 比较了纵向声子与横向声子对磁振子谱的软化与磁振子谱线增宽的影响，也讨论了各项参数 的变化对磁振子谱的软化与磁振子谱线增宽的影响. 关键词： 磁振子-声子相互作用 磁振子软化 铁磁体 磁振子谱线增宽     

组合振子天线磁偶特性实验研究

通过对组合振子的实验研究,验证了磁偶极子回路所具有的优势:能够极大地改善天线低频传输以及辐射特性,具有明显的低频补偿能力。此外,通过设置磁偶回路周长比,比较了不同磁偶回路状态下的天线特性,发现双磁偶回路对于低频特性的改善要优于单磁偶回路,后者的优势主要体现在高频。根据这一现象,采用单磁偶回路结构设计工作频带为300MHz~5GHz组合振子接收天线。     

复合振子天线阵列的数值模拟

 用时域有限差分方法模拟了由复合振子天线单元组成的天线阵列的辐射特性;计算了天线从同轴线的馈电效率,给出了天线阵列的辐射场和能量方向图;比较了不同排列方式下阵列的辐射方向图。模拟结果表明：这种天线阵列具有宽带特性和较高的馈电效率,适合于超宽带电磁脉冲的辐射应用。     

高功率单层径向线螺旋阵列天线的设计与模拟

 在研究磁探针耦合特性的基础上，设计了中心频率为4.0 GHz的3圈36单元高功率单层径向线螺旋阵列天线，各圈距中心位置分别为45，90，135 mm，单元个数分别为6，12，18。该天线采用磁探针代替电探针给短螺旋单元天线馈电，通过同轴-径向线模式转换器实现径向线TEM外行波激励，采用调整磁探针的探入深度和绕轴旋转短螺旋单元天线的方法改变单元的激励幅度与激励相位。数值模拟结果表明：该口径为324 mm的天线在中心频率上可获得21.58 dB的增益，口径效率可达78.2％，轴向轴比值为1.73；在3.8～4.2 GHz的频率范围内增益大于20.85 dB，口径效率大于73.2％，轴向轴比值小于2.0，反射系数小于0.27，辐射效率大于93%。     

FeXXI离子电偶级、磁偶极及电四极跃迁振子强度的计算

讨论了使用MCHF方法优化径向波函数以获取大量原子参数的方法，由得到的波函数计算了FeXXI离子的相对论与非相对论能级，将计算能级与已有的实验结果进行了比较，对电偶极，磁偶极以及电四极的振子强度进行了非相对论与相对论修正的计算，对非相对论计算的振子强度，长度与速度两种表示符合较好。     

The radio-transmitting properties of a carbon nanotube vibrator located on the boundary of a dielectric

The quantum and mechanical properties of a carbon nanotube are described in a model with the use of a macroscopic parameter, viz., surface impedance. Solving the boundary problem for the impedance vibrator is reduced to solving paired integral equations for the vibrator current. The paired integral equations are solved by the Galerkin method with Chebyshev’s basis. The influence of the substrate on the amplitude and frequency characteristics of the antenna, a carbon nanotube, is investigated.     

Simulation of a satellite antenna tuned by a plasma load

We have investigated experimentally and theoretically the effect of a RF discharge excited in a rarefied gas by the antenna field on the input and radiation characteristics of the antenna. Under the conditions of our experiments the discharge plasma is localized near the end of a vibrator antenna, and the parameters of this plasma inhomogeneity can be changed by varying the pressure of the gas, the frequency of the RF signal, and the power fed to the antenna. The excitation of the RF discharge led to the modification of the antenna near field and, as a result, to changes of its electrodynamic characteristics.Nizhnii Novgorod State University. Tranlated from Izvestiya Vysshikh Uchebnykh Zavedenii, Radiofizika, Vol. 37, No. 6, pp. 707–714, June, 1994.     

Comparison of unidirectional signal reception in a waveguide with linear vector-scalar and combined antennas

Experimentally measured spatial responses of linear scalar, vector-scalar, and combined antennas have been analyzed. A combined antenna consists of an extended scalar antenna and one or several vector-scalar modules. It is shown that a combined antenna, which multiplicatively processes signals (just like a vector-scalar antenna), suppresses reflection lobes and provides unidirectional reception (in comparison with a scalar antenna). At the same time, the side field level decreases, thus increasing noise immunity.     

Induced field of an electromagnetic vibrator above a conducting screen placed in a microwave beam

The induced field of a cylindrical electromagnetic vibrator with spherically rounded ends is calculated. The vibrator is above a flat screen placed in a linearly polarized quasi-optical microwave beam. The plane of the screen is perpendicular to the Poynting vector of the radiation. The axis of the vibrator is aligned with the vector of the exciting field electrical component. In calculation, the length of the vibrator and the vibrator-screen distance were varied, while its diameter and the initial field were kept constant. It is found that the induced field of the vibrator with a length close to the half-wavelength of the field is maximal at the ends of the vibrator and the field strength resonantly depends on the length of the vibrator. The shortening of the “half-wavelength” vibrator that provides a maximal induced field is determined. The result of numerical simulation is to an extent intriguing. It is revealed that the induced field of a resonance half-wavelength vibrator rises considerably when the vibrator-screen distance becomes shorter than the quarter-wavelength of the field. The Q factor of an equivalent electromagnetic oscillating circuit characterizing the vibrator also grows, and the induced field more and more concentrates between the screen and the surface of the vibrator’s ends facing the screen. Full-scale experiments qualitatively support theoretical predictions. The results allow researchers to considerably extend the application area of vibrators as initiators of breakdown in high-pressure gases to ignite microwave discharges in quasi-optical beams with a low initial field.     

Microwave breakdown of air initiated by a short electromagnetic vibrator

The electrical breakdown of air (under a pressure from several tens of Torr to several hundreds of Torr) is initiated in a linearly polarized quasi-optical microwave beam using a rounded-end cylindrical metallic electromagnetic vibrator placed parallel to the electric component of the microwave field. The vibrator is much shorter than the wavelength of the field. The field strength at the top of the vibrator as a function of its length is determined. An empiric expression relating the field strength at the top with the vibrator length-to-diameter ratio is found for the vibrator length range studied. The practicability of locally measuring the field in a quasioptical microwave beam is substantiated. The idea is to determine the maximal air pressure at which electrical breakdown of air initiated by a short vibrator placed at a given point of the beam takes place.     

A linear piezoelectric inchworm motor using ultrasonic clamping vibrator

This paper reports a kind of linear piezoelectric inchworm motor us-ing ultrasonic clamping vibrator with ring-shaped three-pile piececonstruction.The clamping vibrator and guide shaft of the motor constitutethe friction pair.The ratio of moving friction coefficient to static one is about1:10,when the clamping vibrator is in resonance.The driving peak voltage ofthe clamping vibrator is only 120V(V_(p-p)).The velocities of the motor are0-2 mm/min,the driving force is about 0.2 kgf,and the mechanic resolvingpower is less than 50nm.The motor's technique is simple.