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CN112993578B - Polarization coding phased array amplitude limiting antenna - Google Patents

Polarization coding phased array amplitude limiting antenna Download PDF

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CN112993578B
CN112993578B CN202110070214.6A CN202110070214A CN112993578B CN 112993578 B CN112993578 B CN 112993578B CN 202110070214 A CN202110070214 A CN 202110070214A CN 112993578 B CN112993578 B CN 112993578B
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antenna
metal
phased array
diode unit
radiation
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CN112993578A (en
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林铭团
徐�明
邓博文
李杨飞
毋召锋
刘培国
刘晨曦
徐延林
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National University of Defense Technology
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q9/00Electrically-short antennas having dimensions not more than twice the operating wavelength and consisting of conductive active radiating elements
    • H01Q9/04Resonant antennas
    • H01Q9/0407Substantially flat resonant element parallel to ground plane, e.g. patch antenna
    • H01Q9/0414Substantially flat resonant element parallel to ground plane, e.g. patch antenna in a stacked or folded configuration
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q23/00Antennas with active circuits or circuit elements integrated within them or attached to them
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q3/00Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system
    • H01Q3/26Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture
    • H01Q3/30Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array
    • H01Q3/34Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array by electrical means

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Abstract

本申请涉及一种极化编码相控阵限幅天线。所述天线包括:编码相控阵天线本体,编码相控阵天线本体包括三层结构,三层结构分别为:第一金属层,包括:第一金属贴片、第二金属贴片以及辐射二极管单元;第一金属贴片和第二金属贴片通过辐射二极管单元连接;第二金属层,包括:金属地面;第三金属层,包括:直流偏置线、馈线和扇形枝节,限幅二极管单元通过过孔与地面相连接;第一金属贴片和第二金属贴片通过过孔与金属地面连接;直流偏置线通过过孔与辐射二极管单元连接。采用本方法能够实现高限幅以及高集成度的编码相控阵天线。

Figure 202110070214

The present application relates to a polarization coded phased array amplitude limiting antenna. The antenna includes: a coded phased array antenna body, the coded phased array antenna body includes a three-layer structure, and the three-layer structures are: a first metal layer, including: a first metal patch, a second metal patch and a radiation diode unit; the first metal patch and the second metal patch are connected through a radiation diode unit; the second metal layer includes: a metal ground; the third metal layer includes: a DC bias line, a feeder line and a fan-shaped branch, and a limiter diode unit The first metal patch and the second metal patch are connected to the metal ground through the via hole; the DC bias line is connected to the radiation diode unit through the via hole. By adopting the method, a coded phased array antenna with high amplitude limiting and high integration can be realized.

Figure 202110070214

Description

一种极化编码相控阵限幅天线A Polarization Coded Phased Array Slicing Antenna

技术领域technical field

本申请涉及雷达技术领域,特别是涉及一种极化编码相控阵限幅天线。The present application relates to the field of radar technology, and in particular, to a polarization-coded phased array amplitude limiting antenna.

背景技术Background technique

传统相控阵天线为实现动态波数扫描,需在T/R组件中使用移相器,从而导致成本、体积的控制困难和系统整体设计复杂等问题。近年提出的反射式和透射式编码超材料天线在此问题上有所改进,其通过加载超材料表面,对入射的电磁波进行调控,可以达到动态波束扫描功能,在一定程度上降低了成本。但也存在设计上的问题,其必须在超材料上方增加空间馈源,用于发射调制波束,从而导致集成困难,天线的加工和实际应用受到影响。In order to achieve dynamic wavenumber scanning, the traditional phased array antenna needs to use a phase shifter in the T/R component, which leads to problems such as difficulty in cost, volume control, and complex overall system design. Reflective and transmissive coded metamaterial antennas proposed in recent years have been improved in this regard. By loading the metamaterial surface and regulating the incident electromagnetic wave, the dynamic beam scanning function can be achieved, which reduces the cost to a certain extent. But there is also a design problem, which must add a space feed above the metamaterial for transmitting modulated beams, which leads to difficulties in integration, and affects the fabrication and practical application of the antenna.

天线作为射频和微波系统前门,是实现自由空间中电磁场与微波电路导行波转换的主要通道,极易受到自然和人为的高强度辐射场的干扰和影响。入射的高强度辐射场经过前门耦合,很可能产生幅度较大的电流,因此与天线相关的电子系统极易受到损伤甚至摧毁。传统的限幅手段,存在系统复杂度高,成本和体积控制困难等问题,难以在集成度和效果方面得到平衡。As the front door of radio frequency and microwave systems, antenna is the main channel to realize the conversion of electromagnetic field and microwave circuit guided traveling wave in free space. The incoming high-intensity radiation field is coupled through the front door, and it is likely to generate a large current, so the electronic system related to the antenna is extremely vulnerable to damage or even destruction. The traditional limiting method has problems such as high system complexity, difficult cost and volume control, etc., and it is difficult to achieve a balance in terms of integration and effect.

发明内容SUMMARY OF THE INVENTION

基于此,有必要针对上述技术问题,提供一种能够平衡相控阵天线集成和限幅问题的一种极化编码相控阵限幅天线。Based on this, it is necessary to provide a polarization-coded phased array amplitude limiting antenna that can balance the problems of phased array antenna integration and amplitude limitation in view of the above technical problems.

一种极化编码相控阵限幅天线,所述方法包括:A polarization-coded phased array amplitude limiting antenna, the method comprising:

极化编码相控阵天线本体,所述编码相控阵天线本体包括三层结构,三层结构分别为:Polarization coding phased array antenna body, the coding phased array antenna body includes a three-layer structure, and the three-layer structures are:

第一金属层,包括:第一金属贴片、第二金属贴片以及辐射二极管单元;所述第一金属贴片和所述第二金属贴片通过辐射二极管单元连接;The first metal layer includes: a first metal patch, a second metal patch and a radiation diode unit; the first metal patch and the second metal patch are connected by a radiation diode unit;

第二金属层,包括:金属地面;The second metal layer, including: metal ground;

第三金属层,包括:直流偏置线、馈线和接地共面波导,限幅二极管单元通过过孔与所述地面相连接;The third metal layer includes: a DC bias line, a feed line and a grounded coplanar waveguide, and the limiting diode unit is connected to the ground through a via hole;

所述第一金属贴片和所述第二金属贴片通过过孔与所述金属地面连接;the first metal patch and the second metal patch are connected to the metal ground through vias;

所述直流偏置线通过过孔与所述辐射二极管单元连接。The DC bias line is connected to the radiation diode unit through a via hole.

在其中一个实施例中,还包括:所述辐射二极管单元包括:两个辐射PIN二极管;所述直流偏置线用于控制所述辐射PIN二极管的导通和截止。In one of the embodiments, it further includes: the radiation diode unit includes: two radiation PIN diodes; the DC bias line is used to control the turn-on and turn-off of the radiation PIN diodes.

在其中一个实施例中,所述第三金属层还包括:扇形枝节;所述扇形枝节刻蚀在所述直流偏置线上。In one embodiment, the third metal layer further includes: a fan-shaped branch; the fan-shaped branch is etched on the DC bias line.

在其中一个实施例中,所述扇形枝节为1/4波长的扇形枝节;所述扇形枝节对称刻蚀在所述直流偏置线的两侧。In one embodiment, the fan-shaped branches are 1/4 wavelength fan-shaped branches; the fan-shaped branches are symmetrically etched on both sides of the DC bias line.

在其中一个实施例中,所述馈线上还刻蚀缝隙和焊接电容,用于阻断控制辐射二极管单元的直流偏置信号。In one embodiment, slits and welding capacitors are further etched on the feeder line, so as to block the DC bias signal for controlling the radiation diode unit.

在其中一个实施例中,所述限幅二极管单元包括:两对限幅PIN二极管;所述两对限幅PIN二极管焊接在接地过孔与馈线之间。In one embodiment, the clipping diode unit includes: two pairs of clipping PIN diodes; the two pairs of clipping PIN diodes are welded between the grounding via and the feeder.

上述一种极化编码相控阵限幅天线,直接在天线单元的两个金属贴片上集成二极管,通过独立辐射,产生两种编码状态稳定的180°相差,实现了对天线辐射波束的1比特数字编码,形成了两种极化。相较于其他编码天线在射频输入上引入相位翻转,具有设计和天线工作简单的优点。另外,应对当前复杂电磁环境,以天线的限幅能力为出发点,通过设置限幅二极管单元将限幅功能集成于相控阵天线设计中,使相控阵天线具备限幅能力。从而实现极化编码相控阵限幅天线。The above-mentioned polarized coding phased array limiting antenna directly integrates diodes on the two metal patches of the antenna unit, and generates a stable 180° phase difference between the two coding states through independent radiation, and realizes the 180° phase difference of the antenna radiation beam. Bits are digitally encoded, forming two polarizations. Compared with other coded antennas that introduce phase inversion on the RF input, it has the advantages of simple design and antenna operation. In addition, to cope with the current complex electromagnetic environment, taking the amplitude limiting ability of the antenna as the starting point, the amplitude limiting function is integrated into the design of the phased array antenna by setting the limiting diode unit, so that the phased array antenna has the amplitude limiting ability. Thereby, the polarization-encoded phased array amplitude limiting antenna is realized.

附图说明Description of drawings

图1为一个实施例中第一金属层的示意性结构图;FIG. 1 is a schematic structural diagram of a first metal layer in one embodiment;

图2为一个实施例中第二金属层的示意性结构图;FIG. 2 is a schematic structural diagram of a second metal layer in one embodiment;

图3为一个实施例中第三金属层的示意性结构图3 is a schematic structural diagram of a third metal layer in one embodiment

图4为一个实施例中极化编码相控阵限幅天线的侧视图;4 is a side view of a polarization-encoded phased array limiting antenna in one embodiment;

图5为一个实施例中加载限幅二极管天线E面方向图;FIG. 5 is a pattern of the E-plane of the loaded limiting diode antenna in one embodiment;

图6为一个实施例中加载限幅二极管天线H面方向图;FIG. 6 is an H-plane pattern of a loaded limiting diode antenna in one embodiment;

图7为一个实施例中未加载限幅二极管天线E面方向图;7 is an E-plane pattern of an unloaded limiting diode antenna in one embodiment;

图8为一个实施例中未加载限幅二极管天线H面方向图;8 is an H-plane pattern of an unloaded limiting diode antenna in one embodiment;

图9为一个实施例中码相控阵限幅天线单元的S参数仿真图;9 is an S-parameter simulation diagram of a coded phased array limiting antenna unit in one embodiment;

图10为一个实施例中天线单元在编码“0”时的电场分布图;FIG. 10 is an electric field distribution diagram of the antenna element when encoding "0" in one embodiment;

图11为一个实施例中天线单元在编码“1”时的电场分布图;Fig. 11 is the electric field distribution diagram of the antenna element when coding "1" in one embodiment;

图12为一个实施例中10°使用和未使用随机相位的波束扫描方向图对比;FIG. 12 is a comparison of beam scanning patterns with and without random phase at 10° in one embodiment;

图13为一个实施例中各个扫描角度的波束扫描方向图;FIG. 13 is a beam scan pattern of each scan angle in one embodiment;

图14为一个实施例中限幅二极管导通时的波束扫描方向图。FIG. 14 is a beam scanning direction diagram when the limiting diode is turned on in one embodiment.

具体实施方式Detailed ways

为了使本申请的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本申请进行进一步详细说明。应当理解,此处描述的具体实施例仅仅用以解释本申请,并不用于限定本申请。In order to make the purpose, technical solutions and advantages of the present application more clearly understood, the present application will be described in further detail below with reference to the accompanying drawings and embodiments. It should be understood that the specific embodiments described herein are only used to explain the present application, but not to limit the present application.

在一个实施例中,提供了一种极化编码相控阵限幅天线,包括:编码相控阵天线本体,编码相控阵天线本体包括三层结构,三层结构分别为:第一金属层、第二金属层以及第三金属层。In one embodiment, a polarization-coded phased array amplitude limiting antenna is provided, including: a coded phased array antenna body, the coded phased array antenna body includes a three-layer structure, and the three-layer structures are: a first metal layer , a second metal layer and a third metal layer.

如图1所示,第一金属层包括:第一金属贴片101、第二金属贴片102以及辐射二极管单元103;第一金属贴片101和第二金属贴片102通过辐射二极管单元103连接。As shown in FIG. 1 , the first metal layer includes: a first metal patch 101 , a second metal patch 102 and a radiation diode unit 103 ; the first metal patch 101 and the second metal patch 102 are connected through the radiation diode unit 103 .

如图2所示,第二金属层包括:金属地面201。As shown in FIG. 2 , the second metal layer includes: a metal ground 201 .

如图3所示,第三金属层包括:直流偏置线301和馈线302,限幅二极管单元303通过接地共面波导304与地面201相连接,隔直流电容305焊接在馈线302之上。As shown in FIG. 3 , the third metal layer includes a DC bias line 301 and a feeder line 302 , the limiting diode unit 303 is connected to the ground 201 through a grounded coplanar waveguide 304 , and a DC blocking capacitor 305 is welded on the feeder line 302 .

第一金属贴片101和第二金属贴片102通过过孔与金属地面201连接。The first metal patch 101 and the second metal patch 102 are connected to the metal ground 201 through via holes.

直流偏置线301通过过孔与辐射二极管单元103连接。The DC bias line 301 is connected to the radiation diode unit 103 through a via hole.

上述一种极化编码相控阵限幅天线,直接在天线单元的两个金属贴片上集成二极管,通过独立辐射,产生两种编码状态稳定的180°相差,实现了对天线辐射波束的1比特数字编码。相较于其他编码天线在射频输入上引入相位翻转,具有设计和天线工作简单的优点。另外,应对当前复杂电磁环境,以天线的限幅能力为出发点,通过设置限幅二极管单元将限幅功能集成于相控阵天线设计中,使相控阵天线具备限幅能力。从而实现编码相控阵限幅天线。The above-mentioned polarized coding phased array limiting antenna directly integrates diodes on the two metal patches of the antenna unit, and generates a stable 180° phase difference between the two coding states through independent radiation, and realizes the 180° phase difference of the antenna radiation beam. Bit number coding. Compared with other coded antennas that introduce phase inversion on the RF input, it has the advantages of simple design and antenna operation. In addition, to cope with the current complex electromagnetic environment, taking the amplitude limiting ability of the antenna as the starting point, the amplitude limiting function is integrated into the design of the phased array antenna by setting the limiting diode unit, so that the phased array antenna has the amplitude limiting ability. Thus, a coded phased array limiting antenna is realized.

在其中一个实施例中,辐射二极管单元包括:两个辐射PIN二极管,直流偏置线用于控制辐射PIN二极管的导通和截止。本实施例中,两个金属贴片上集成PIN二极管,通过独立辐射,产生两种编码状态稳定的180°相差,实现了对天线辐射波束的1比特数字编码。相较于其他编码天线在射频输入上引入相位翻转,具有设计和天线工作简单的优点。另一方面,仅在两个金属贴片上集成PIN二极管,就具备了编码波束扫描能力,较传统相控阵天线在输入射频信号上做文章,简化了扫描波束形成机制,易于设计、加工和推广。In one of the embodiments, the radiation diode unit includes: two radiation PIN diodes, and a DC bias line is used to control the turn-on and turn-off of the radiation PIN diodes. In this embodiment, PIN diodes are integrated on two metal patches, and through independent radiation, a phase difference of 180° with stable two encoding states is generated, and 1-bit digital encoding of the antenna radiation beam is realized. Compared with other coded antennas that introduce phase inversion on the RF input, it has the advantages of simple design and antenna operation. On the other hand, only integrating PIN diodes on two metal patches has the ability to scan coded beams. Compared with traditional phased array antennas, it makes a fuss about the input RF signal, simplifies the scanning beamforming mechanism, and is easy to design, process and promotion.

在其中一个实施例中,第三金属层还包括:扇形枝节306;扇形枝节306刻蚀在直流偏置线上。本实施例中,即便有少量射频信号流入直流偏置线,经过扇形枝节后也将被短路,不会进入直流馈线端。In one embodiment, the third metal layer further includes: a fan-shaped branch 306; the fan-shaped branch 306 is etched on the DC bias line. In this embodiment, even if a small amount of radio frequency signal flows into the DC bias line, it will be short-circuited after passing through the fan-shaped branch, and will not enter the DC feeder end.

作为一个具体实现,扇形枝节为1/4波长的扇形枝节,扇形枝节对称刻蚀在直流偏置线的两侧。As a specific implementation, the fan-shaped branches are 1/4 wavelength fan-shaped branches, and the fan-shaped branches are symmetrically etched on both sides of the DC bias line.

在其中一个实施例中,馈线上还刻蚀缝隙和焊接电容305,用于阻断控制辐射二极管单元的直流偏置信号。本实施例中,消除直流偏置信号对限幅PIN二极管的影响。In one of the embodiments, a slit and a welding capacitor 305 are also etched on the feeder line to block the DC bias signal for controlling the radiation diode unit. In this embodiment, the influence of the DC bias signal on the limiting PIN diode is eliminated.

在其中一个实施例中,限幅二极管单元包括:两对限幅PIN二极管;两对限幅PIN二极管焊接在在接地共面波导304缝隙与馈线302之间。本实施例中,应对当前复杂电磁环境,以天线的限幅能力为出发点,通过设置限幅二极管单元将限幅功能集成于相控阵天线设计中,使相控阵天线具备限幅能力。从而实现编码相控阵限幅天线。In one embodiment, the clipping diode unit includes: two pairs of clipping PIN diodes; the two pairs of clipping PIN diodes are welded between the gap of the grounded coplanar waveguide 304 and the feeder 302 . In this embodiment, in response to the current complex electromagnetic environment, the amplitude limiting capability of the antenna is taken as the starting point, and the amplitude limiting function is integrated into the phased array antenna design by setting the amplitude limiting diode unit, so that the phased array antenna has the amplitude limiting capability. Thus, a coded phased array limiting antenna is realized.

综上所述,通过引入PIN二极管,将限幅功能集成在系统前端,舍弃了复杂繁重的移相器和移相控制网络,实现了天线和限幅一体化。另一方面,将PIN二极管集成在天线单元上面,就使其具备限幅能力,且限幅二极管加载不影响天线的性能指标。To sum up, by introducing a PIN diode, the limiter function is integrated in the front end of the system, and the complex and heavy phase shifter and phase shift control network are abandoned, and the integration of the antenna and the limiter is realized. On the other hand, integrating the PIN diode on the antenna unit makes it capable of clipping, and the loading of the clipping diode does not affect the performance index of the antenna.

具体的,如图4所示,是本发明一种极化编码相控阵限幅天线的侧视图,结合图1-4,设计极化编码相控阵限幅天线,需要完成图中如下参数的设计:L1、L2、L3、R1、R2、R3、W1、W2、W3、W4、H1、H2。L1为金属贴片长度;L2为限幅PIN二极管间距;L3天线单元长度;R1为过孔半径;R2为扇形枝节半径;R3为中间过孔半径;W1为金属贴片宽度;W2为直流偏置线宽度;W3为馈线宽度;W4为天线宽度;H1为介质层1厚度;H2为介质层2厚度。Specifically, as shown in FIG. 4, it is a side view of a polarization-encoded phased array limiting antenna according to the present invention. With reference to FIGS. 1-4, to design a polarization-encoded phased array limiting antenna, the following parameters in the figure need to be completed. Design: L1, L2, L3, R1, R2, R3, W1, W2, W3, W4, H1, H2. L1 is the length of the metal patch; L2 is the limiter PIN diode spacing; L3 is the length of the antenna unit; R1 is the radius of the via hole; R2 is the radius of the sector branch; R3 is the radius of the intermediate via; W1 is the width of the metal patch; W2 is the DC bias W3 is the width of the feeder; W4 is the width of the antenna; H1 is the thickness of the dielectric layer 1; H2 is the thickness of the dielectric layer 2.

以下通过几组实验数据对本发明的有益效果进行说明。The beneficial effects of the present invention will be described below through several sets of experimental data.

1、对极化编码相控阵限幅天线单元方向图的仿真。1. Simulation of the pattern of the polarized coding phased array limiting antenna element.

如图5-8所示,分别是加载限幅二极管天线E面方向图、加载限幅二极管天线H面方向图、未加载限幅二极管天线E面方向图以及未加载限幅二极管天线H面方向图。As shown in Figure 5-8, the pattern of the E surface of the loaded limiter diode antenna, the pattern of the H surface of the loaded limiter diode antenna, the pattern of the E surface of the unloaded limiter diode antenna, and the direction of the H surface of the unloaded limiter diode antenna are respectively picture.

如图5和6所示,分别描绘了当限幅二极管处于通态和截止状态时天线方向图的E平面和H平面。仿真结果表明,该天线具有近-20dB的限幅效果。可以看到,当高强度电磁辐射场入射导致限幅二极管导通时,方向图增益明显减小,这意味着该天线与自由空间阻抗不匹配,无法从外部接收能量。因此,当天线受到强场辐射时,可以获得很好的限幅性能。图7和8为不加载限幅二极管时天线方向图的E平面和H平面。将图7和8与图5和6限幅二极管截止时的E面和H面方向图对比,可以看到限幅二极管加载前后,天线方向图没有变化,说明限幅二极管的加载与否对天线方向图没有影响。As shown in Figures 5 and 6, the E-plane and H-plane of the antenna pattern are depicted when the clipping diode is in the on and off states, respectively. Simulation results show that the antenna has a clipping effect of nearly -20dB. It can be seen that when the high-intensity electromagnetic radiation field is incident and the limiting diode is turned on, the pattern gain is significantly reduced, which means that the antenna does not match the free space impedance and cannot receive energy from the outside. Therefore, when the antenna is radiated by a strong field, a good amplitude limiting performance can be obtained. Figures 7 and 8 show the E-plane and H-plane of the antenna pattern when the limiting diode is not loaded. Comparing Figures 7 and 8 with Figures 5 and 6 when the limiting diodes are turned off, it can be seen that the antenna pattern does not change before and after the limiting diode is loaded, indicating whether the loading of the limiting diode affects the antenna. The orientation map has no effect.

2、对编码相控阵限幅天线单元的S参数仿真。2. S-parameter simulation of coded phased array limiting antenna unit.

如图9所示,限幅二极管在截止状态时,S11参数在-10dB下的带宽为0.5GHz,相对带宽为5.5%。而当限幅二极管在导通状态时,该天线的反射系数趋于0dB,也就是说高强度辐射场被反射。该仿真证实了限幅二极管导通时,本设计可以明显增强天线对高强度辐射场的反射。同时在限幅二极管截止时,可以保证天线的正常性能不受影响。As shown in Figure 9, when the limiting diode is in the cut-off state, the bandwidth of the S11 parameter at -10dB is 0.5GHz, and the relative bandwidth is 5.5%. And when the limiting diode is in the conducting state, the reflection coefficient of the antenna tends to 0dB, that is to say, the high-intensity radiation field is reflected. The simulation confirms that this design can significantly enhance the antenna's reflection to high-intensity radiated fields when the limiting diode is turned on. At the same time, when the limiting diode is turned off, the normal performance of the antenna can be guaranteed not to be affected.

3、极化编码相控阵限幅天线单元场分布图3. Field distribution diagram of polarized coding phased array limiting antenna unit

如图10和11所示,分别表示天线单元在“0”和“1”两个不同编码时的电场分布图。从场分布图可以很清楚的看到,当天线处于不同的编码状态时,电场的方向相反。即当天线处于不同编码状态时,天线的极化方向相反。As shown in Figs. 10 and 11, the electric field distribution diagrams of the antenna element under two different codes of "0" and "1" are respectively shown. It is clear from the field distribution diagram that the direction of the electric field is opposite when the antenna is in different coding states. That is, when the antennas are in different coding states, the polarization directions of the antennas are opposite.

4、极化编码相控阵限幅天线一维阵列图。4. One-dimensional array diagram of polarization-encoded phased array limiting antenna.

如图12-14所示,为编码相控阵限幅天线阵列的波束扫描方向图。由图12所示,1比特阵列天线在波束形成时,容易在形成较大的副瓣。为减小副瓣,馈电时给每个天线单元设置初始相位差,并在仿真时引入随机相位,如图12可见副瓣压制效果较好,可达24.2dB。图13为分别在0°、10°、20°、30°时的方向图,天线主波束角度精度较高。图14为限幅二极管导通时,天线进入限幅状态,此时天线不工作。比较图13、14在对应偏转角度的增益,可以发现图14对应角度的增益比图13减小34.2dB。说明在限幅二极管导通后,天线进入限幅状态,显示出较好的限幅效果。Figure 12-14 shows the beam scanning pattern of the coded phased array limiting antenna array. As shown in FIG. 12 , when the 1-bit array antenna is beam-forming, it is easy to form large side lobes. In order to reduce the side lobes, the initial phase difference is set for each antenna element during feeding, and a random phase is introduced during the simulation. As shown in Figure 12, the side lobe suppression effect is better, up to 24.2dB. Figure 13 shows the directional diagrams at 0°, 10°, 20°, and 30° respectively, and the angle of the main beam of the antenna is highly accurate. Figure 14 shows that when the limiting diode is turned on, the antenna enters the limiting state, and the antenna does not work at this time. Comparing the gain at the corresponding deflection angle in Figs. 13 and 14, we can find that the gain at the corresponding angle in Fig. 14 is 34.2dB lower than that in Fig. 13. It shows that after the limiting diode is turned on, the antenna enters the limiting state, showing a better limiting effect.

以上实施例的各技术特征可以进行任意的组合,为使描述简洁,未对上述实施例中的各个技术特征所有可能的组合都进行描述,然而,只要这些技术特征的组合不存在矛盾,都应当认为是本说明书记载的范围。The technical features of the above embodiments can be combined arbitrarily. For the sake of brevity, all possible combinations of the technical features in the above embodiments are not described. However, as long as there is no contradiction in the combination of these technical features, all It is considered to be the range described in this specification.

以上所述实施例仅表达了本申请的几种实施方式,其描述较为具体和详细,但并不能因此而理解为对发明专利范围的限制。应当指出的是,对于本领域的普通技术人员来说,在不脱离本申请构思的前提下,还可以做出若干变形和改进,这些都属于本申请的保护范围。因此,本申请专利的保护范围应以所附权利要求为准。The above-mentioned embodiments only represent several embodiments of the present application, and the descriptions thereof are specific and detailed, but should not be construed as a limitation on the scope of the invention patent. It should be pointed out that for those skilled in the art, without departing from the concept of the present application, several modifications and improvements can be made, which all belong to the protection scope of the present application. Therefore, the scope of protection of the patent of the present application shall be subject to the appended claims.

Claims (5)

1. A polarization encoded phased array limited antenna, the antenna comprising:
polarization encoding phased array antenna body, polarization encoding phased array antenna body includes three layer construction, and three layer construction is respectively:
a first metal layer comprising: the radiation diode comprises a first metal patch, a second metal patch and a radiation diode unit; the first metal patch and the second metal patch are connected through a radiation diode unit;
a second metal layer comprising: a metal floor;
a third metal layer comprising: the amplitude limiting diode unit is connected with the ground through a through hole;
the clipping diode unit includes: two pairs of amplitude limiting PIN diodes; the two pairs of amplitude limiting PIN diodes are welded between the gap of the grounded coplanar waveguide and the feeder line;
the first metal patch is connected with the metal ground through a via hole;
the direct current bias line is connected with the radiation diode unit through a via hole.
2. The antenna of claim 1, wherein the radiating diode unit comprises: two radiating PIN diodes;
the direct current bias line is used for controlling the conduction and the cut-off of the radiation PIN diode.
3. The antenna of claim 1, wherein the third metal layer further comprises: fan-shaped branch knots;
the fan-shaped branch knot is etched on the direct current bias line.
4. The antenna of claim 3, wherein the sector stub is a sector stub of 1/4 wavelengths;
the fan-shaped branches are symmetrically etched on two sides of the direct current bias line.
5. The antenna of claim 3 or 4, wherein the feed line is further etched with a gap and a solder capacitor for blocking a DC bias signal for controlling the radiation diode unit.
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