带状注行波管双矩形螺旋线慢波结构高频特性北大核心CSCD

针对新型螺旋线慢波结构——双矩形螺旋线慢波结构,即在金属屏蔽框内平行加载两个具有矩形横截面形状的自由螺旋线慢波结构,利用三维电磁仿真软件对其高频特性(色散特性和耦合阻抗)进行模拟研究。结果表明:在相同位置处,与单矩形螺旋线慢波结构相比,双矩形螺旋线慢波结构色散特性变化很小,却有着更高的耦合阻抗;同时,在包含这些位置的空间部分,可采用带状电子注与该慢波结构进行注波互作用,使输出功率进一步得到提高。     

螺旋线厚度对螺旋线慢波结构高频特性的影响

在螺旋坐标系下采用近似场匹配法研究了厚度较厚的螺旋线慢波结构的高频特性,得到了其色散方程,并数值计算了螺旋线厚度对慢波系统的相速的影响。结果表明:随螺旋线厚度的增加,慢波结构的色散曲线变得平坦,色散变弱,带宽增加。与软件仿真结果及Hook的螺旋线模型对比表明:采用近似场匹配法的计算结果与CST仿真吻合得更好,比Hook模型具有更高的准确性,从而证明所采用理论方法的有效性。     

基于场匹配法的双排矩形栅慢波结构高频特性研究

本文运用场匹配法对具有任意位错的双排矩形栅慢波结构的场分布、色散特性及耦合阻抗进行了研究．研究结果表明,场匹配法推导的色散特性与仿真软件CST和HFSS计算的结果完全一致,耦合阻抗介于CST和HFSS之间．在此基础上,详细研究了上下两排系统之间位错对色散特性及耦合阻抗的影响．当位错严格为半个周期时,第一阻带消失,第一个模式最高截止频率与第二个模式最低截止频率重叠,发生简并;当位错为0．45倍周期时,在保证耦合阻抗不变的情况下,基模的通带虽降低了2．8GHz,但阻带却增大了7．9GHz,从而可以有效避免简并及模式竞争的发生．     

具有任意槽的矩形波导栅慢波结构高频特性的研究

将任意形状槽的连续轮廓近似用一系列相连的矩形阶梯近似，利用各阶梯面上导纳的匹配，以及槽与互作用区边界场的连续与匹配条件，获得了具有任意槽的矩形波导栅慢波结构的色散方程和耦合阻抗的表达式，并进行理论上的验证.加工制作了矩形槽波导栅模型，冷测表明理论值与测量值相吻合.分别求解几种特殊槽形矩形波导栅慢波结构的色散特性及耦合阻抗，其中，三角形结构的色散和耦合阻抗均最弱，而倒梯形结构色散最强，耦合阻抗最大. 关键词： 矩形波导栅 任意槽 色散特性 慢波结构     

等离子体加载螺旋线行波管特性研究

利用线性场理论和螺旋线的导电面模型，推导了在强引导磁场下，等离子体加载螺旋线慢波结构的色散关系.数值计算了在不同的等离子体填充密度与填充半径条件下，螺旋线的色散特性、耦合阻抗和行波管的小信号增益.研究发现，在螺旋线中填充了等离子体以后，形成了一种新的混合模式，螺旋线的色散特性与耦合阻抗都发生了很大的变化，行波管的增益得到显著提高. 关键词： 螺旋线行波管 等离子体 混合模式     

阶梯槽交错双栅慢波结构高频特性理论和模拟

本文基于一种阶梯槽交错双栅周期慢波结构模型,获得了该结构中的电磁场分布公式.通过场匹配方法,求出了该结构的高频色散方程和耦合阻抗表达式.以W波段行波管用的阶梯槽交错双栅为例,利用本文公式和CST-MWS电磁软件比较计算了色散和耦合阻抗特性,分析了阶梯尺寸参数对高频特性(基模色散、+1次空间谐波归一化相速和耦合阻抗)的影响.结果表明,理论和CST-MWS软件模拟有很好的一致性;相对矩形交错双栅,改善了色散特性,拓展了基模带宽,同时具有足够大的耦合阻抗和适合工程应用的机械强度,在一定程度上可以弥补矩形交错双栅周期慢波结构的不足.     

Chodorow型耦合腔慢波结构色散特性和耦合阻抗理论分析

本文建立了Chodorow型耦合腔慢波结构的解析模型, 利用并矢格林函数结合矩量法求解了场匹配方程, 给出了色散方程和耦合阻抗的计算式, 并数值计算出一个X波段Chodorow型慢波结构的高频特性. 结果表明, 本文方法的色散特性以及耦合阻抗与仿真软件HFSS计算的结果有很好的一致性, 且计算效率更高, 同时精度远高于等效电路法, 对工程设计有好的参考价值. 关键词： Chodorow型耦合腔慢波结构 色散特性 耦合阻抗 场匹配     

同轴任意槽形周期圆波导慢波结构色散特性的研究

用阶梯近似的方法分析任意槽形加载的圆波导慢波系统，利用各阶梯相邻面的导纳匹配条件 以及中心互作用区与加载区的场匹配条件，获得了任意槽形加载周期慢波结构的统一色散方 程. 利用该色散方程，得到色散特性与CST MWS仿真软件模拟结果良好符合. 分别求解几种 特殊槽形加载慢波结构的色散特性及耦合阻抗，其中，三角形结构色散和耦合阻抗均最弱， 而倒梯形结构色散最强，耦合阻抗最大. 关键词： 任意槽形 慢波结构 色散特性 行波管     

矩形栅慢波系统的高频特性分析

对于矩形栅这一经典的慢波结构，采用场匹配法来分析其慢波特性，进而得到其耦合阻抗。其中对槽区内的场处理，保留其高次项，表示为一无限本征驻波之和的形式。然后通过数值实例具体分析了矩形栅的两种典型结构:浅槽栅和深槽栅。当增大槽深后，色散增强，系统通带变窄，同时耦合阻抗有明显增大，工作点移向前向波区，适合用在放大器的慢波结构上。     

螺旋线径向挤压变形对其慢波结构冷测特性的影响

 介绍了用MAFIA软件的准周期边界条件计算螺旋线行波管慢波结构的色散和耦合阻抗，以及用ANSYS软件对螺旋线径向挤压变形建模的方法，并对螺旋线受挤压径向变形对其冷测特性的影响进行了详细的分析。结果表明:螺旋线径向挤压变形会导致相速增大，而在通常的变形范围内耦合阻抗也会增加；当变形继续增大时耦合阻抗上升到最大值后开始下降。     

Acoustical fields from rectangular ultrasonic transducers for non-destructive testing and medical diagnosis

Theoretical results are given for pressure and intensity in the acoustical field produced by rectangular ultrasonic transducers. Comparison between the fields of square, circular and rectangular transducers is made showing that the field of a rectangular transducer, by comparison with that produced by square and circular transducers, may be divided into three zones rather than two: the very nearfield, the nearfield and the farfield. Some experimental results are shown confirming the general shape of the predicted curves. Emphasis is put on the difficulty of interpreting quantitative ultrasonic results with rectangular probes.     

LO-phonon effect on the exciton binding energy in polar rectangular quantum wires

Longitudinal optical phonon effect on Wannier excitons in polar rectangular quantum wires is studied by a variational approach. The binding energy is calculated and the numerical results for several II-VI and III-V compound semiconductor rectangular quantum wires are given. The results show that the phonon effect reduces the binding energy and cannot be neglected. The phonon contribution to the binding energy is sensitive to the size of the rectangular quantum wire section, and increases with decreasing section area. The results for the GaAs rectangular quantum wires coincide with the experimental results. The calculated binding energy and the phonon effect in II-VI QWWs are both stronger than those in III-V compound systems, and the results for ZnSe QWW are qualitatively in agreement with the experiments.     

悬臂方薄板振动的辐射声场及竖裂纹对其频谱的影响

在将悬臂板挠度表示为正交多项式之和的基础上，利用瑞利-里兹方法求解了悬臂板的前几阶振动模态频率及挠度．进而利用瑞利积分求解了其自由振动辐射声场的分布规律。用分区技术的瑞利-里兹方法求解了竖裂纹对悬臂板低阶模态频率的影响，并将计算结果与有限元结果作了对照。实验上用小球撞击法测定了含竖裂纹悬臂板辐射声场的频谱，谱成分与有限元结果基本符合。     

矩形波导栅慢波系统的实验研究

 从实验上研究了矩形波导栅慢波系统的色散特性及其耦合装置的驻波系数，用分布加工的方法分别制作了矩形、燕尾形、梯形3种不同槽形的矩形波导栅慢波结构模型和带输入输出结构的矩形波导栅慢波结构实体模型。采用谐振法测量它们的色散特性和驻波系数，实验结果与理论计算值和模拟值吻合良好。     

Tees on partially filled rectangular waveguides

We propose an analytical solution of the problem of determination of external parameters of T-shaped E and H tees on partially filled rectangular waveguides. The solution is tested for a particular case of E and H tees on hollow rectangular waveguides and compared with the known solution obtained by the numerical method. Calculated results show good agreement. Numeral results are given for tees on partially filled rectangular waveguides.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Radiofizika, Vol. 39, No. 7, pp. 901–909, July, 1996.     

H-在矩形腔中的光剥离截面

根据半经典闭合轨道理论研究了矩形腔对氢负离子的光剥离进程的影响,利用反射定律分析矩形腔中与光剥离截面相联系的剥离电子运动的闭合轨道,推导出该体系下的光剥离截面公式,在线性极化光的作用下,研究了腔的尺寸对光剥离截面的影响,并将其与麻志君等用量子力学方法研究的结果进行对比.结果表明:矩形腔的存在及其大小对光剥离截面中由闭合轨道相联系的返回波与波源函数发生干涉引起的振荡有很大影响,且振荡曲线随着矩形腔的尺寸变化明显;当激光极化方向沿着x轴或者y轴时,半经典方法与量子力学方法的结果一致,当激光极化方向沿着Z轴时,由于矩形腔在z轴上对光剥离截面不作用,采用半经典方法光剥离截面与无场的情况相同,但是采用量子力学方法,其结果中却出现振荡,表明半经典方法研究此体系结果更准确.研究结果可对研究负离子光剥离以及外腔中的电子输运问题提供参考.     

矩形槽同轴布拉格结构的模式匹配分析方法及实验验证

基于模式匹配法建立了矩形槽同轴布拉格结构的全波耦合分析模型, 推导出了不同模式反射率和传输率的计算式, 并采用公开报道的实验数据验证了该理论模型. 在此基础上就本文理论与其他相关的理论方法进行了比较, 发现以前的理论近似模型由于忽略了矩形槽中的消失模而使传输率的频率响应曲线发生偏差. 本文建立的理论方法有望为矩形槽同轴布拉格结构的特性研究和工程实践提供一种理论分析手段. 关键词： 同轴布拉格结构 矩形波纹 模式匹配法 模式耦合     

Capacitance and surface charge distribution computations for a satellite modeled as a rectangular cuboid and two plates

This paper presents a method to evaluate the capacitance and the surface charge distributions of a satellite modeled as a structure consisting of a rectangular cuboid with two coplanar rectangular plates. The Charges accumulate on the satellite surfaces result destructive electrostatic discharges (ESD). Integral equations are formed by relating the unknown charge density on the metallic cuboid and the two rectangular plates to the potential on the surface of these bodies. The integral equations are solved using the Method of Moments (MoM) based on pulse function as basis functions and delta functions as testing functions. In order to apply MoM, the surfaces of the metallic bodies are discretized by using non-uniform rectangular subsections. The numerical data on capacitance of this structure have been presented. The key results are that the computational method is validated by computing the capacitance of a cuboid to be 73.46 pF/m, which is consistent with previous works. Faster convergence and shorter computational time are achieved using non-uniform subsections. And, as expected, the surface charge density diminishes at joints where the plates connect to the cuboid.     

Fano resonance in asymmetric gold nano-dimers with square and rectangular sections

The Fano resonances of the asymmetric dimers of gold nanowires with square and rectangular sections are investigated by using the finite-difference time-domain (FDTD) method. It is found that the Fano resonance peak can be switched on and off by laying or removing the rectangular section nanowire aside the square section one. There is only one dipole resonance mode of a single gold nanowire with a square section on the dielectric substrate, and it redshifts obviously accompanied with the FWHM being broadened along with the side width of the nanowire increasing. A Fano resonance appears when another gold nanowire with the rectangular section is laid aside the one with a square section. The peak value and FWHM of the Fano resonance mode increase obviously with the distance between the two nanowires getting larger. Meanwhile, it can be modulated by the height of the rectangular section nanowire. In addition, they can be regulated by the width and rotating angle of the rectangular section nanowire, but the peak value stays the same. The mechanisms for these behaviors are associated with the interaction of the superradiant and subradiant modes, and the corresponding electric field distributions are plotted to verify this. It is expected that the results will be useful for the design of wavelength biosensing and other new optical devices.     

Localization of Surface Plasmon Waves in Hybrid Photodetectors with Subwavelength Metallic Arrays

The spectral characteristics of the hole photocurrent in plasmon photodetectors based on Ge/Si heterostructures with Ge quantum dots combined with regular arrays of subwavelength apertures of various shapes in a gold film on the semiconductor surface are investigated. Dispersion relations characterizing the propagation of surface plasmon waves along the metal–semiconductor interface are determined from the dependences of the photocurrent on the angle of incidence of light. It is established that the plasmonic enhancement of the photocurrent in rectangular aperture array is suppressed as compared to that in circular and square aperture arrays. It is found that, in hybrid structures with rectangular apertures, there exists a range of wave vectors where the energy of surface plasmons is independent of the wave vector of incident radiation. The results are explained by the excitation of dipole modes localized at rectangular apertures with a large aspect ratio by light waves.