一种新型双环双模带通滤波器

本文提出了一种由一个环形谐振器和一个微扰小环构成的新型双环双模带通滤波器。微扰小环具有两个可调参数,增加了调整双模的自由度,从而更容易地调节双模,便于实现滤波器的小型化。抽头输入输出耦合结构可以方便地调整双模滤波器的两个传输零点,从而改善滤波器的通带特性。最后实现了中心频率为2.41GHz,相对带宽为17.77%的双环双模带通滤波器,通带内插入损耗为0.67dB,回波损耗为17dB,且带外衰减大于20dB。     

基于频率变换的双通带腔体滤波器的研究

该文基于频率变换的方法设计了两种结构的双通带的腔体滤波器,一种是通过谐振器之间直接耦合实现的;另一种是在谐振器之间引入交叉耦合实现的,从而达到产生传输零点的目的。首先根据设计指标,采用频率变换的方法,计算得到谐振器间的耦合系数和外部Q值,然后利用Ansoft HFSS建立同轴腔体滤波器的模型并进行仿真,仿真结果与ADS中等效电路得到的理论结果基本吻合,从而验证了这种方法的正确性。最后通过对级联型结构与交叉耦合型结构双通带腔体滤波器的比较,得出后者比前者具有更好的带外抑制特性。     

一种基于微带开口环的双通带滤波器设计

文中提出了一种基于微带开口环的双通带滤波器设计,对比了非对称开口环结构与传统对称结构的传输特性,讨论了非对称结构中两端馈线位置,双环耦合间距以及环线宽度对于滤波器性能的影响,然后在此基础上,利用两级级联耦合开口环设计了一个用于接收机中抑制镜像的双通带滤波器,带外抑制度较高。     

基于枝节线加载谐振器的可调滤波器设计

传统基于变容二极管的双频电可调滤波器由于外部容值的加入,该类滤波器的插损变大,同时相对带宽锐减。基于多模谐振器结构,提出了一种新型的工作频段独立、电可调的双频带通滤波器。该滤波器由短路枝节线加载谐振器和一对1/4 波长谐振器组成。在各自的谐振器末端加载带有变容二极管的外部偏置电路,1/4 波长谐振器构成第一通带,短路枝节线加载谐振器构成第二通带,两通带之间互不干扰,单独调节。应用奇偶模分析法及调节耦合间距的方法,确保双通带均出现两个极点,保证其带宽的稳定性。该电可调滤波器第一通带可调范围为0.7 ~0.85 GHz,第二通带可调范围为0.9 ~1.05 GHz,同时双频带的相对带宽基本保持在10% 以上,较以往的双频电可调滤波器,该款滤波器的相对带宽有了较为明显的提升。     

高选择性吸收式可调带阻滤波器的研究

该研究利用耦合相消原理设计了一种吸收式可调带阻滤波器.在传统耦合相消结构的基础上,提出了一种新的结构,通过增加耦合结构的阶数以及增大耦合支路中谐振器的电长度,使得滤波器阻带特性的Q值增大,从而提高了滤波器的选择性.通过调节加载在谐振器上变容二极管的偏置电压,实现滤波器带阻中心频率可调.并对实测结果和仿真结果进行了探讨.     

2.45 GHz宽阻带高抑制腔体滤波器的研究设计

针对手持式谐波雷达发射机自身产生的谐波信号严重干扰接收到的探测目标谐波信号问题,该文设计了一种谐振器开路端加圆盘的结构,该结构能有效缩小滤波器体积和抑制高次谐振频率产生的寄生通带,并研究了圆盘半径、谐振杆长度、调谐螺钉长度和半径对腔体滤波器谐振频率的影响。结果表明,圆盘半径和调谐螺钉半径增大,则等效电容增加,谐振频率降低。忽略其他因数影响,随着谐振杆长度和调谐螺钉长度增加,等效电感增大,谐振频率降低。最后,利用HFSS软件优化设计了一款中心频率2.45 GHz、带宽0.1 GHz的腔体滤波器。测试结果表明,滤波器通带内插损小于1 dB,阻带为3~9 GHz内衰减优于90 dB,体积仅为51 mm×11 mm×27 mm,满足设计要求。     

基于横向滤波器理论的小型超宽带差分带通滤波器

 本文提出了一种基于横向滤波器理论的小型超宽带差分滤波器结构.由于输入/输出端口之间具有两条不同电长度的传输路径,使得差模信号的通带两端具有两个传输零点并且具有良好的谐波抑制特性.四条1/4波长的短路线被用来改善差模信号的通带特性.另外,共模信号可以很容易在整个频段上得到抑制.加工结构模型的测试结果表明:差模信号的相对带宽为102%,带内的回波损耗大于15dB.实验测试结果与理论仿真结果吻合较好.     

同轴腔带通滤波器的一种设计方法

采用负阻线子网络…构造了多腔耦合的同轴带通滤波器电路模型，应用电路分析软件对滤波器进行了分析优化，得到腔体之间耦合系数和接入点位置。应用三维全波分析软件，分析了腔体结构参数与耦合系数和耦合窗的关系。以这种路和场的仿真、优化相结合的方法，得出了滤波器的耦合和输入输出结构参数。运用该方法设计的中心频率2．4GHz，通带100MHz的六腔滤波器的实际测试结果与仿真分析结果基本一致。     

传输矩阵法分析多环高阶谐振滤波器特性

与输入／输出波导耦合的环型谐振腔能形成结构简洁、性能良好、集成度高的信道滤波器。为实现通带内频率响应平坦度高、滚降时间快的滤波效果,采用多环结构形成的高阶滤波器。利用传输矩阵法推导了环与环问通过串联耦合和并联耦合两种方式形成的多环高阶谐振滤波器的传输甬数公式。对于并联耦合结构,通过优化直接影响下话路滤波特性的环与环间直波导的长度,实现了下话路光谱的对称性。对于串联结构,影响其特性的主要因素为环与环间的耦合系数．要实现最大平坦的通带特性,通过数值计算得出各个环间耦合系数必须从中间到两侧对称增加的特性。     

新型紧凑型带通滤波器的设计

文章设计了两个通带位于超宽带低频范围的带通滤波器,用一种T型结构来代替传统带通滤波器中的四分之一波长传输线,这种替代减小了滤波器的尺寸.而且,可以很方便的控制位于滤波器通带两端的传输零点,即合理的调节开路支线的电长度,进而可以方便的控制滤波器的通带范围.为了证明以上新型滤波器的优点,设计了两个开路支线电长度不同的带通滤...     

宽带接收机应用的超宽倍频程电调滤波器设计*

电调谐预选滤波器是宽带接收机的关键部件,直接影响到整机性能的好坏。设计了一种采用梳状滤波结构的电调滤波器,工作频段为200~600MHz,整个调谐范围内,1d B带宽约为12%,插入损耗小于3d B,输入二阶截点值大于60d Bm,输入三阶截点值大于20d Bm,输入输出端口驻波比小于1.8,测试和仿真结果吻合良好。该滤波器结构简单、体积小、工艺上易实现,还具有超宽倍频程的调谐范围及低插损、高截点值等优良电性能。     

基于HFSS设计同轴腔调谐滤波器

同轴腔调谐滤波器在军事通信设备中具有广泛应用.论述了该类滤波器的设计原理,详细分析了腔间耦合孔和输入、输出耦合环的位置和大小的设计,在此基础上应用高频结构仿真软件(HFSS),对L波段调谐滤波器的实例进行仿真设计.结果表明仿真拟合准确,说明应用HFSS仿真软件能够很好的描述调谐滤波器的关键设计内容.     

一种采用螺旋耦合环的同轴腔可调滤波器

提出了一种采用螺旋耦合环的小型化连续可调的同轴腔可调滤波器.对比传统的单一窗口耦合结构,加入螺旋耦合环可以显著地减小可调滤波器在整个工作频率范围内的带宽变化.采用螺旋耦合环可使可调滤波器插入损耗指标获得进一步改善,并可利用它对滤波器带宽在一定范围内进行调节.基于这种耦合结构设计了一个3腔可调滤波器,并对其传输特性进行了...     

A new electronically tunable current mode universal filter using MO-CCCII

A new electronically tunable universal current mode biquad filter structure employing three multiple output current controlled conveyors (MOCCCII) and two grounded capacitors is presented. The proposed filter offers the following advantageous features: low input impedance and high output impedance—a desirable property of current mode filters; realization of low pass, band pass, high pass, notch, and all pass; no matching constraint; low sensitivity performance and use of grounded capacitors suitable for integration. The practical design problems due to nonlinearities of MOCCCIIs have also been addressed. The feasibility of the design is confirmed via SPICE simulations.     

Design and Simulation of a Narrow Passband Electro-Optical Tunable Filter with Band-pass and Band-rejection Output

An electro-optical tunable filter comprised of two paralleled identical long-period waveguide gratings is proposed in this paper. The filter has one input port and two separate output ports, outputting band-pass and band-rejection light respectively. Using poled electro-optical polymer material to fabricate its waveguide cores enable the filter’s tuning speed to approach nanosecond order. With the aid of long-period waveguide gratings, the tuning range of the filter is Λ times larger than the conventional electro-optical filters. We built up a model to design and simulate the proposed tunable optical filter. We investigate the relationship between the parameters of the long-period waveguide grating and the characteristics of the tunable filter, such as tuning range and FWHM. The simulation results show that the tunable optical filter can realize high-speed tuning in the wavelength range of 1530 nm to 1560 nm, and the FWHM width can reach 0.8 nm. Compared with the conventional optical filters, the results show that a high-speed widely tunable optical filter with narrow pass band can be achieved.     

Tunable notch filter using a thermooptic long-period grating

This paper proposes a tunable notch filter using a thermooptic long-period grating and investigates it theoretically. This notch filter is in the form of an integrated optical device and is based on a simple structure as compared with existing integrated optical notch filters. The thermooptic grating denotes a thermooptic index perturbation induced by periodic heaters. The attenuation of a resonance band in the transmission spectrum of the proposed notch filter can be controlled by adjusting the electric power applied to the periodic heaters. Employing the heat transfer theory and the coupled-mode theory, the proposed filter is designed and analyzed. The paper also presents analytic expressions for the temperature change due to a heater and the coupling coefficients due to the thermooptic grating. This filter may have potential as a compact dynamically controllable device like a tunable gain flattening filter.     

Electronically Tunable Microwave Bandpass Filters

Combline filters with novel input and output coupling networks which enable broad-band tuning to be achieved with minimum degradation in passband performance are discussed. Explicit design formulas for these filters are presented. Computer analysis of varactor tuned combine bandpass filters including the small signal varactor equivalent circuit is presented enabling filter performance to be easily evaluated. The design and experimental performance of a varactor tuned combline filter, realized in suspended substrate stripline is described. This filter toned from 3.2 GHz to 4.9 GHz exhibited low passband insertion loss and its performance was is close agreement with theoretical expectations.     

基于激光外调制的频率可调谐光电振荡器

为了实现光电振荡器(OEO)输出频率的可调谐,提出了一种基于外调制激光的频率可调谐光电振荡器。此方案在单环OEO的基础上增加一个由微波滤波器、电衰减器、电放大器和电移相器构成的电增益选频腔,通过调节电移相器的偏置电压可以等效改变电选频腔的腔长,从而改变其输出微波信号的频率;同时调节光延时线来改变光电振荡器的起振模式,通过电增益选频腔信号与光电振荡器自由振荡信号的电注入锁定,即可实现频率可调谐的光电振荡器,其输出信号的频率由锁定OEO模式的电增益选频腔决定。实验结果表明,本方案产生了频率调谐范围为10.05 GHz~10.09 GHz、调谐步长为400 kHz的输出信号,频率在40 MHz的范围内连续可调谐。在输出频率为10.0519 GHz时,其边模抑制比为60 dB,相位噪声为-115 dBc/Hz @10 kHz。该方案结构简单,既保留了单环OEO低相位噪声的优势,又能有效抑制边模,为实现频率可调谐OEO提供了一种新的方法。     

An original approach to the design of bandpass cavity filters withmultiple couplings

A novel approach to the design of general cavity filters with each cavity coupled to an arbitrary number of other cavities is presented. This approach is based on a suitable characterization of the filter structure which does not require one to model separately the cavities (resonators) and the coupling elements. Suitably defined equivalent admittances are associated with each cavity allowing one to design the filter structure once the parameters of a suitable low-pass prototype are given; an efficient procedure for the synthesis of such a prototype with equiripple passband response is also presented which allows one to arbitrarily prescribe transmission zeros placed in the complex plane (even asymmetrically). The described design approach is particularly convenient when the filter structure does not allow a simple modeling of the resonators and coupling elements separately. This is the case of slot-coupled cavity filters and of filter structures based on arrays of coupled transmission lines. It is also shown that the simplified design approach often adopted in the past, where only two coupled cavities at a time are considered, can produce large errors even in the case of filters with all attenuation poles at infinity (i.e., two couplings per cavity)