CN103972623B - A kind of waveguide filter based on electromagnetic induced transparency - Google Patents
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Abstract
本发明公开了一种基于电磁感应透明的波导滤波器,其结构包括构成标准矩形波导的上腔体、下腔体、插入到标准矩形波导上腔体和下腔体之间的介质基板、信号输入端口和信号输出端口,介质基板正面的金属微带结构有矩形金属环、带外抑制片、两排金属化通孔和接地外延带,介质基板背面的金属微带结构有两个对称C形谐振结构以及接地外延带。位于介质基板正面的矩形金属环和位于介质基板背面的两个对称C形谐振结构相互作用产生电感应透明窗和磁感应透明窗的两个通带,即形成电磁感应透明效应,利用该效应实现的波导滤波器,其通带的上下边带各有一个传输零点,具有较高的选择性,而且结构紧凑易于设计。
The invention discloses a waveguide filter based on electromagnetic induction transparency. Input ports and signal output ports, the metal microstrip structure on the front of the dielectric substrate has a rectangular metal ring, an out-of-band suppression sheet, two rows of metallized through holes and grounding extension strips, and the metal microstrip structure on the back of the dielectric substrate has two symmetrical C-shaped resonant structure and grounded epitaxy. The rectangular metal ring on the front of the dielectric substrate and the two symmetrical C-shaped resonant structures on the back of the dielectric substrate interact to produce two passbands of the inductive transparent window and the magnetic inductive transparent window, that is, the electromagnetic induction transparent effect is formed. The waveguide filter has a transmission zero in the upper and lower sidebands of the passband, has high selectivity, and is compact and easy to design.
Description
技术领域technical field
本发明涉及微波毫米波滤波器设计技术,尤其涉及一种波导型滤波器设计的新方法。The invention relates to microwave and millimeter wave filter design technology, in particular to a new method for waveguide filter design.
背景技术Background technique
波导滤波器由于其损耗小,功率容量大等优点在很多微波、毫米波系统中得到了广泛的应用。有多种实现技术,例如直接耦合谐振腔,消逝模波导滤波器,多模波导滤波器以及E面波导滤波器等。其中直接耦合谐振腔设计方法,虽然设计灵活,且矩形系数好,损耗小,但是其加工较复杂,成本高,不易进行大批量生产。而E面波导滤波器加工简单、成本低、适用于大批量生产,设计较灵活,但是传统的E面波导滤波器为了得到优良的滤波器性能必须进行多级两联,这不可以避免的造成滤波器的整体尺寸较大。当然研究学者们也做了必要的改进研究,其中有E面双膜片的插入(见F.Arndt,J.Bornemann,R.Vahldieck,et al.E-plane IntegratedCircuit Filters with Improved Stopband Attenuation(short Papers)[J].Microwave Theory and Techniques,IEEE Transactionson,1984,32(10),1391-1394.)虽然改善了其滤波器的阻带特性,但这种其仍需要进行多级级联,体积仍然相对较大。另外,虽然国内的研究进展相对落后一些,但仍有一些新研究成果,2009年吴卫涛、梁昌洪、翟博韬和温海宾对加载周期性脊波导的E面滤波器(见吴卫涛,梁昌洪,翟博韬,等.加载周期性脊波导的E面滤波器[C],2009年全国微波毫米波会议,2009,51-52.)进行了研究,该滤波器基于E面膜片波导滤波器,提出了一种具有高选择性的滤波器实现方案,将插有E面膜片的波导和脊波导组合在一起,在E面膜片滤波器的半波谐振器中间嵌入周期性的脊波导结构。该E面波导滤波器克服了传统滤波器的缺点,具有带外衰减快、尺寸较传统的E面波导滤波器小的特点,当然我们也看到在其设计过程中不可避免的进行了多级级联。Waveguide filters have been widely used in many microwave and millimeter wave systems due to their small loss and large power capacity. There are various implementation techniques such as direct coupled resonators, evanescent mode waveguide filters, multimode waveguide filters, and E-plane waveguide filters. Among them, the direct coupling resonant cavity design method has flexible design, good square coefficient and low loss, but its processing is more complicated, the cost is high, and it is not easy to carry out mass production. The E-plane waveguide filter is simple to process, low in cost, suitable for mass production, and more flexible in design, but the traditional E-plane waveguide filter must be multi-staged in order to obtain excellent filter performance, which inevitably causes The overall size of the filter is larger. Of course, researchers have also made necessary improvements, including the insertion of double diaphragms on the E-plane (see F. Arndt, J. Bornemann, R. Vahldieck, et al. E-plane Integrated Circuit Filters with Improved Stopband Attenuation (short Papers )[J].Microwave Theory and Techniques,IEEE Transactionson,1984,32(10),1391-1394.) Although the stopband characteristics of its filter have been improved, this kind of filter still needs to be cascaded in multiple stages, and the volume is still relatively bigger. In addition, although domestic research progress is relatively backward, there are still some new research results. In 2009, Wu Weitao, Liang Changhong, Zhai Botao and Wen Haibin studied the E-plane filter loaded with periodic ridge waveguide (see Wu Weitao, Liang Changhong, Zhai Botao, etc. The E-plane filter loaded with periodic ridge waveguide [C], 2009 National Microwave and Millimeter Wave Conference, 2009, 51-52.) conducted research, the filter is based on the E-film sheet waveguide filter, and proposed a high A selective filter implementation scheme combines the waveguide and the ridge waveguide inserted with the E-mask sheet filter, and embeds a periodic ridge waveguide structure in the middle of the half-wave resonator of the E-mask sheet filter. The E-plane waveguide filter overcomes the shortcomings of traditional filters, and has the characteristics of fast out-of-band attenuation and smaller size than traditional E-plane waveguide filters. cascade.
在E面波导滤波器的设计中,不可避免的需要进行多级级联从而造成体积增大,因此有必要研究并设计一种新型的波导滤波器,使其采用较小的结构尺寸实现较好的滤波性能。In the design of the E-plane waveguide filter, multi-level cascading is inevitably required to increase the volume, so it is necessary to study and design a new type of waveguide filter to achieve better performance with a smaller structural size. filtering performance.
而电磁感应透明EIT(Electromagnetically induced transparency)效应是量子学方面的一个重要研究点,通常传输媒质因电磁感应透明效应特性而产生的一个信号可传输通带很窄。很多基于EIT效应的应用表现在量子学领域。近年来,有学者研究可以采用集总电路元件,开口谐振环等非量子学的结构实现EIT效应(见郭晓莹,杨靖,李建,等.RLC电路中类电磁感应透明现象的实验研究[J].山西大学学报(自然科学版),2012(1):68-74。)。The EIT (Electromagnetically induced transparency) effect is an important research point in quantum science. Usually, the transmittable passband of a signal generated by the transmission medium due to the characteristics of the electromagnetically induced transparency effect is very narrow. Many applications based on the EIT effect appear in the field of quantum science. In recent years, some scholars have studied that non-quantum structures such as lumped circuit components and split resonant rings can be used to realize the EIT effect (see Guo Xiaoying, Yang Jing, Li Jian, et al. Experimental research on electromagnetic induction-like transparency in RLC circuits[J ]. Shanxi University Journal (Natural Science Edition), 2012(1): 68-74.).
由于EIT效应可以产生一个透明通带的特性,因此可以想象采用这种电磁感应透明EIT效应是可以设计带通滤波器的。因此,本发明将采用EIT效应设计一种新型的E面波导滤波器,其具有高矩形系数,损耗小,结构紧凑,设计灵活等优点。这种将在这种量子学领域的电磁感应透明(EIT)效应有效的应用于毫米波频段波导滤波器设计中,将丰富滤波器设计理念,增加新理论,将为滤波器等器件设计提供一定的理论基础,具有理论与实践指导意义。Since the EIT effect can produce a transparent passband characteristic, it is conceivable that a bandpass filter can be designed using this electromagnetically induced transparent EIT effect. Therefore, the present invention will use the EIT effect to design a novel E-plane waveguide filter, which has the advantages of high squareness coefficient, small loss, compact structure, and flexible design. This kind of electromagnetic induction transparency (EIT) effect in this field of quantum science is effectively applied to the design of waveguide filters in the millimeter wave band, which will enrich the concept of filter design, add new theories, and provide a certain degree for the design of filters and other devices. It has theoretical and practical guiding significance.
发明内容Contents of the invention
为了改善E面波导滤波器的性能,在已有的研究设计中都进行了多级级联,不可避免造成了体积相对较大的缺陷,因此有必要发明一种新型的E面波导滤波器,使其克服对级联的需求,采用较小的结构尺寸实现较好的滤波性能。In order to improve the performance of the E-plane waveguide filter, multi-level cascading has been carried out in the existing research design, which inevitably caused relatively large defects. Therefore, it is necessary to invent a new type of E-plane waveguide filter. It overcomes the need for cascading, and achieves better filtering performance with a smaller structure size.
为了实现上述目的,本发明的技术方案是:In order to achieve the above object, technical scheme of the present invention is:
一种基于电磁感应透明的波导滤波器,包括构成标准矩形波导的上腔体(1)、下腔体、插入到标准矩形波导上腔体和下腔体之间的介质基板、信号输入端口和信号输出端口;所述介质基板正面的金属微带结构有矩形金属环、带外抑制片、两排金属化通孔和接地外延带,介质基板背面的金属微带结构有两个对称C形谐振结构以及接地外延带;A waveguide filter based on electromagnetic induction transparency, comprising an upper cavity (1) constituting a standard rectangular waveguide, a lower cavity, a dielectric substrate inserted between the upper cavity and the lower cavity of the standard rectangular waveguide, a signal input port and Signal output port; the metal microstrip structure on the front of the dielectric substrate has a rectangular metal ring, an out-of-band suppression sheet, two rows of metallized through holes and a grounding epitaxial strip, and the metal microstrip structure on the back of the dielectric substrate has two symmetrical C-shaped resonances structure and ground extension strip;
通过调节矩形金属环和两个对称C形谐振结构的结构尺寸,使其在某一频带内产生强的相互作用进而生成电感应透明窗和磁感应透明窗的两个通带窗口,即形成电磁感应透明效应;利用该效应实现的波导滤波器,其通带的上下边带各有一个传输零点。其具体设计为,合理设计矩形金属环和两个对称C形谐振结构的尺寸大小,使得调节电感应透明窗和磁感应透明窗的两个通带的位置,使两个透明通带接近并交叠,从而形成具有优良性能的带通滤波特性,实现基于EIT概念的波导滤波器,由于电磁感应透明窗是由电谐振和磁谐振产生的,因此在滤波器透明通带的上下边带各引入了一个传输零点,有效的提高了波导滤波器的矩形系数;By adjusting the structural size of the rectangular metal ring and two symmetrical C-shaped resonant structures, they can generate a strong interaction in a certain frequency band and then generate two passband windows of the electric induction transparent window and the magnetic induction transparent window, that is, form the electromagnetic induction Transparency effect; the waveguide filter realized by using this effect has a transmission zero in the upper and lower sidebands of the passband. Its specific design is to reasonably design the size of the rectangular metal ring and the two symmetrical C-shaped resonant structures, so that the positions of the two passbands of the electric induction transparent window and the magnetic induction transparent window are adjusted, so that the two transparent passbands are close to and overlap , so as to form a band-pass filtering characteristic with excellent performance, and realize a waveguide filter based on the EIT concept. Since the electromagnetic induction transparent window is produced by electric resonance and magnetic resonance, the upper and lower sidebands of the transparent passband of the filter are respectively introduced. A transmission zero effectively improves the square coefficient of the waveguide filter;
信号输入端口和输出端口直接由标准矩形波导构成,信号不需要经过任何金属微带结构过渡直接由输入端口作用到介质基板正反面的金属微带结构上,然后由输出端口输出;介质基板背面的两个对称C形谐振结构,其C型的上下臂长可以从0mm开始变化,从而可以灵活的调节并设计电感应透明通带和磁感应透明通带的位置;The signal input port and output port are directly composed of standard rectangular waveguides, and the signal does not need to pass through any metal microstrip structure transition directly from the input port to the metal microstrip structure on the front and back of the dielectric substrate, and then output from the output port; the back of the dielectric substrate Two symmetrical C-shaped resonant structures, the length of the upper and lower arms of the C-shaped can be changed from 0mm, so that the position of the inductively induced transparent passband and the magnetically induced transparent passband can be flexibly adjusted and designed;
介质基板正面的具有一定带外抑制作用的带外抑制片经由基板外延带与波导的上下波导壁直接相连接,其宽度取值可以为0mm;位于介质基板反面的接地外延带与介质基板正面的接地外延带结构尺寸相同,并通过两排金属化通孔相连。在设计中应注意,当矩形金属环的占空比较小时可以合理设计带外抑制片,可改善其该电磁感应透明的波导滤波器的阻带抑制性能,而当矩形金属环的占空比较大时,该结构将会很小,其改善的性能受限,因此为设计简单可以去掉该结构,也即宽度变为了0。The out-of-band suppression sheet with a certain out-of-band suppression effect on the front of the dielectric substrate is directly connected to the upper and lower waveguide walls of the waveguide through the substrate epitaxial tape, and its width can be 0 mm; The grounded epitaxy structures are of the same size and are connected by two rows of metallized vias. It should be noted in the design that when the duty ratio of the rectangular metal ring is small, the out-of-band suppression sheet can be designed reasonably, which can improve the stop-band suppression performance of the electromagnetic induction transparent waveguide filter, and when the duty ratio of the rectangular metal ring is large When , the structure will be very small, and its improved performance is limited, so the structure can be removed for simplicity of design, that is, the width becomes 0.
本发明采用了在具有低损耗的标准金属矩形波导,由上下腔体和构成,在其E面插入介质基板,介质基板正面的矩形金属环结构产生一个被称低Q模的本征模,该模式由矩形金属环与外部输入场的耦合效应产生,产生较强烈的吸收,即在标准矩形波导可内产生一个较宽的阻带,在相同的谐振频点上,矩形金属环的高度越大时品质因数越低,因此在本实用新型设计中应选择阻带的品质因数较低为好。介质基板背面的两个对称C形谐振结构结合介质基板正面的矩形金属环相互作用,在有输入场的情况下产生了电谐振和磁谐振,它们分别对应具有较高的品质因数的电感应透明通带和磁感应透明通带,即电磁感应透明效应,另外,由于电磁感应透明通带的本质是电磁谐振的作用,因此根据电磁谐振的理论,就会有在电感应透明通带的下边带和磁感应透明通带的上边带各出现一个零点的特性,这两个零点对设计具有高矩形系数的波导滤波器有着很重要的影响。合理设计矩形金属环和两个对称C形谐振结构,其中两个对称C形谐振结构上下臂长的L的值可以是从0开始变化的,我们就可以得到符合要求的带通EIT波导滤波器。另外在设计中,我们要特别注意,使电感应透明通带位于磁感应透明通带的下边带,并且调节结构尺寸,可以使得两个原本分开的电磁感应透明通带接近并交叠成一个具有更宽频带的电磁感应透明通带。最后,具有一定带外抑制作用的带外抑制片,在设计中可以灵活应用,当矩形金属环的占空比较小时可以合理设计带外抑制片,可改善其该电磁感应透明的波导滤波器的阻带抑制性能,而当矩形金属环的占空比较大时,该结构将会很小,其改善的性能受限,因此为设计简单可以去掉该结构,也即宽度变为了0。The present invention adopts a standard metal rectangular waveguide with low loss, which is composed of upper and lower cavities and a dielectric substrate is inserted into its E surface, and the rectangular metal ring structure on the front of the dielectric substrate produces an eigenmode called a low-Q mode. The mode is generated by the coupling effect of the rectangular metal ring and the external input field, resulting in stronger absorption, that is, a wider stop band can be generated in the standard rectangular waveguide. At the same resonance frequency point, the greater the height of the rectangular metal ring The lower the quality factor, the lower the quality factor of the stop band should be selected in the design of the utility model. The two symmetrical C-shaped resonant structures on the back of the dielectric substrate interact with the rectangular metal ring on the front of the dielectric substrate to generate electrical resonance and magnetic resonance in the presence of an input field, which correspond to the inductively transparent transparent Pass band and magnetic induction transparent pass band, that is, the effect of electromagnetic induction transparency. In addition, since the essence of electromagnetic induction transparent pass band is the effect of electromagnetic resonance, according to the theory of electromagnetic resonance, there will be a lower sideband and The upper sideband of the magnetically induced transparent passband has a characteristic of zero points, and these two zero points have a very important influence on the design of waveguide filters with high squareness coefficients. Reasonably design a rectangular metal ring and two symmetrical C-shaped resonant structures, where the value of L of the upper and lower arm lengths of the two symmetrical C-shaped resonant structures can change from 0, and we can obtain a bandpass EIT waveguide filter that meets the requirements . In addition, in the design, we should pay special attention to make the inductive induction transparent passband be located in the lower sideband of the magnetic induction transparent passband, and adjust the structure size, so that the two originally separated electromagnetic induction transparent passbands can approach and overlap to form a more transparent passband. Broadband electromagnetic induction transparent passband. Finally, the out-of-band suppression sheet with a certain out-of-band suppression effect can be flexibly applied in the design. When the duty ratio of the rectangular metal ring is small, the out-of-band suppression sheet can be designed reasonably, which can improve the performance of the electromagnetic induction transparent waveguide filter. Stop band suppression performance, and when the duty ratio of the rectangular metal ring is large, the structure will be small, and its improved performance is limited, so the structure can be removed for simplicity of design, that is, the width becomes 0.
本发明的优点和有益效果:Advantage of the present invention and beneficial effect:
(1)本发明采用电磁感应透明(EIT)概念设计的波导滤波器设计,具有高矩形系数、小型化等优良性能。(1) The present invention adopts the waveguide filter design of electromagnetic induction transparency (EIT) concept design, which has excellent performances such as high square coefficient and miniaturization.
(2)本发明采用矩形环、带外抑制金属片及两个对称C形谐振结构,其结构简单,设计灵活方便,且易于设计。(2) The present invention adopts a rectangular ring, an out-of-band suppressing metal sheet and two symmetrical C-shaped resonant structures. The structure is simple, the design is flexible and convenient, and it is easy to design.
(3)本发明采用的与波导壁直接相连接的带外抑制片具有一定的带外抑制优化作用,且设计灵活。(3) The out-of-band suppression sheet directly connected to the waveguide wall used in the present invention has a certain optimization function of out-of-band suppression and is flexible in design.
(4)相对于传统的波导滤波器设计方法,本发明采用新的设计理念,将EIT效应成功用于波导滤波器的设计中,实现性能优良的波导滤波器。(4) Compared with the traditional waveguide filter design method, the present invention adopts a new design concept, successfully applies the EIT effect to the waveguide filter design, and realizes a waveguide filter with excellent performance.
附图说明Description of drawings
下面结合附图及具体实施方式对本发明作进一步的详细说明。The present invention will be further described in detail below in conjunction with the accompanying drawings and specific embodiments.
图1是本发明提供的基于电磁感应透明波导滤波器的结构三维示意图。Fig. 1 is a three-dimensional schematic diagram of the structure of the transparent waveguide filter based on electromagnetic induction provided by the present invention.
图2是本发明提供的基于电磁感应透明的波导滤波器的基板正面结构示意图。Fig. 2 is a schematic diagram of the front structure of the substrate of the waveguide filter based on electromagnetic induction transparency provided by the present invention.
图3是本发明提供的基于电磁感应透明的波导滤波器的基板背面结构示意图。Fig. 3 is a schematic diagram of the backside structure of the substrate of the waveguide filter based on electromagnetic induction transparency provided by the present invention.
图4是本发明提供的基于电磁感应透明的波导滤波器实例的仿真及测试结果对比图。Fig. 4 is a comparison diagram of simulation and test results of an example of a waveguide filter based on electromagnetic induction transparency provided by the present invention.
具体实施方式detailed description
如图1、图2、图3所示,一种基于电磁感应透明的波导滤波器,包括构成标准矩形波导的上腔体1、下腔体2、插入到标准矩形波导上腔体1和下腔体2之间的介质基板3、信号输入端口4和信号输出端口5;所述介质基板3正面的金属微带结构有矩形金属环31、带外抑制片32、两排金属化通孔33和接地外延带34,介质基板3背面的金属微带结构有两个对称C形谐振结构35以及接地外延带36;As shown in Figure 1, Figure 2, and Figure 3, a waveguide filter based on electromagnetic induction transparency includes an upper cavity 1 and a lower cavity 2 that constitute a standard rectangular waveguide, and are inserted into the upper cavity 1 and the lower cavity of the standard rectangular waveguide. The dielectric substrate 3 between the chambers 2, the signal input port 4 and the signal output port 5; the metal microstrip structure on the front of the dielectric substrate 3 has a rectangular metal ring 31, an out-of-band suppression sheet 32, and two rows of metallized through holes 33 and a grounded epitaxial strip 34, the metal microstrip structure on the back of the dielectric substrate 3 has two symmetrical C-shaped resonant structures 35 and a grounded epitaxial strip 36;
介质基板3正面的矩形金属环31和位于介质基板3背面的两个对称C形谐振结构35相互作用产生电谐振透明窗和磁谐振透明窗的两个通带,从而形成电磁感应透明效应;利用该效应实现的波导滤波器,其通带的上下边带各有一个传输零点;The rectangular metal ring 31 on the front of the dielectric substrate 3 and the two symmetrical C-shaped resonant structures 35 on the back of the dielectric substrate 3 interact to generate two passbands of the electric resonance transparent window and the magnetic resonance transparent window, thereby forming an electromagnetic induction transparent effect; The waveguide filter realized by this effect has a transmission zero in the upper and lower sidebands of the passband;
通过调节矩形金属环31和两个对称C形谐振结构35的结构尺寸,使其在某一频带内产生强的相互作用进而生成电感应透明窗和磁感应透明窗的两个通带窗口,即形成电磁感应透明效应;利用该效应实现的波导滤波器,其通带的上下边带各有一个传输零点。By adjusting the structural dimensions of the rectangular metal ring 31 and the two symmetrical C-shaped resonant structures 35, they generate a strong interaction in a certain frequency band and then generate two passband windows of the electric induction transparent window and the magnetic induction transparent window, namely forming Electromagnetic induction transparency effect; the waveguide filter realized by using this effect has a transmission zero point in the upper and lower sidebands of the passband.
信号输入端口4和输出端口5直接由标准矩形波导构成,信号不需要经过任何金属微带结构过渡直接由输入端口4作用到介质基板3正反面的金属微带结构上,然后由输出端口5输出;介质基板3背面的两个对称C形谐振结构35,其C型的上下臂长可以从0mm开始变化;The signal input port 4 and output port 5 are directly composed of standard rectangular waveguides, the signal does not need to pass through any metal microstrip structure transition, and is directly applied to the metal microstrip structure on the front and back of the dielectric substrate 3 by the input port 4, and then output by the output port 5 ; Two symmetrical C-shaped resonant structures 35 on the back of the dielectric substrate 3, the length of the C-shaped upper and lower arms can be changed from 0mm;
介质基板3正面的具有一定带外抑制作用的带外抑制片32经由基板外延带34与波导的上下波导壁直接相连接,其宽度取值可以为0mm;位于介质基板3反面的接地外延带36与介质基板3正面的接地外延带34结构尺寸相同,并通过两排金属化通孔33相连。The out-of-band suppression sheet 32 with a certain out-of-band suppression effect on the front of the dielectric substrate 3 is directly connected to the upper and lower waveguide walls of the waveguide via the substrate extension tape 34, and its width can be 0 mm; It has the same structural size as the ground extension strip 34 on the front surface of the dielectric substrate 3 , and is connected through two rows of metallized through holes 33 .
作为一个实例,一种基于电磁感应透明的波导滤波器被设计、加工、实验。标准矩形波导为工作于Ka波段的WR-28(7.112mm*3.556mm),仿真设计中选用的介质基板为Rogers RT/duroid5880其介电常数为2.2,厚度0.254mm,损耗角正切为0.0009,其中介质基板上的电路结构尺寸分别为,矩形金属环31的高度为3mm,宽度为2mm,基板背面的对称C形谐振结构35的高度为3mm,且对称C形谐振结构35的外边缘间距为2mm,L的值和带外抑制片的宽度为0mm,所有金属条带的宽度为0.2mm。测试结果表明,采用电磁感应透明(EIT)效应设计的新型波导滤波器,具有较高的矩形系数,损耗低,带外抑制优良,且加工成本低,易于大批量生产,且该中波导滤波器设计灵活方便。另外,仿真和实测中的误差主要是由于实验中所采用的基板介电常数在Ka波段并不是恒定不变的2.2的一个常数,其值实际小于2.2,另外由于加工精度,实际操作等因素,造成了测试结果频率向高频偏移。As an example, a waveguide filter based on electromagnetic induction transparency is designed, fabricated, and tested. The standard rectangular waveguide is WR-28 (7.112mm*3.556mm) working in the Ka band. The dielectric substrate selected in the simulation design is Rogers RT/duroid5880 with a dielectric constant of 2.2, a thickness of 0.254mm, and a loss tangent of 0.0009, where The dimensions of the circuit structure on the dielectric substrate are respectively, the height of the rectangular metal ring 31 is 3mm, the width is 2mm, the height of the symmetrical C-shaped resonant structure 35 on the back of the substrate is 3mm, and the distance between the outer edges of the symmetrical C-shaped resonant structure 35 is 2mm , the value of L and the width of the out-of-band suppression sheet are 0mm, and the width of all metal strips is 0.2mm. The test results show that the new waveguide filter designed with the electromagnetic induction transparency (EIT) effect has a high square coefficient, low loss, excellent out-of-band suppression, low processing cost, and is easy to mass-produce, and the waveguide filter The design is flexible and convenient. In addition, the error in simulation and actual measurement is mainly due to the fact that the dielectric constant of the substrate used in the experiment is not a constant of 2.2 in the Ka band, and its value is actually less than 2.2. In addition, due to factors such as processing accuracy and actual operation, The frequency of the test results is shifted to high frequency.
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