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CN108470973B - Broadband RCS (radio control system) reduced super surface based on gap loading - Google Patents

Broadband RCS (radio control system) reduced super surface based on gap loading Download PDF

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CN108470973B
CN108470973B CN201810193433.1A CN201810193433A CN108470973B CN 108470973 B CN108470973 B CN 108470973B CN 201810193433 A CN201810193433 A CN 201810193433A CN 108470973 B CN108470973 B CN 108470973B
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amc
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patch
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square frame
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CN108470973A (en
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葛越
陈嘉卿
陈晓锋
于步云
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Nanjing University of Aeronautics and Astronautics
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/12Supports; Mounting means
    • H01Q1/18Means for stabilising antennas on an unstable platform
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q15/00Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
    • H01Q15/24Polarising devices; Polarisation filters 

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Abstract

The invention discloses a gap loading-based broadband RCS (radio communication system) reduction super surface, which comprises a medium substrate, a metal patch loading gaps and a metal floor, wherein the metal patch loading a plurality of pairs of cross-shaped gaps is printed on the upper surface of the medium substrate, the metal floor is printed on the lower surface of the medium substrate, the resonance frequency of a designed artificial magnetic conductor unit is 12GHz, the in-phase reflection relative bandwidth is 50%, meanwhile, the broadband AMC super unit and another double-ring AMC super unit are arranged at intervals in a 3X 3 chessboard form, each AMC super unit consists of 3X 3 basic AMC units, and finally, the RCS reduction of more than 7.5dB in the frequency range of 8-19.2GHz is realized. The artificial magnetic conductor structure and the AMC-AMC checkerboard electromagnetic stealth surface have the advantages of good robustness, insensitivity to polarization and the like.

Description

基于缝隙加载的宽带RCS缩减超表面Broadband RCS reduced metasurface based on gap loading

技术领域Technical field

本发明涉及雷达隐身技术领域,尤其涉及一种基于缝隙加载的宽带RCS缩减超表面。The invention relates to the field of radar stealth technology, and in particular to a wideband RCS reduced metasurface based on gap loading.

背景技术Background technique

随着探测技术和电磁隐身技术的飞速发展,隐身特性逐渐成为衡量飞行目标性能优劣的重要指标,缩减目标的雷达散射截面(Radar Cross Section,RCS)成为了现代战争中能够先发制人的关键因素。传统的隐身技术主要通过改变飞行目标外形和涂覆雷达吸波材料(RAM)实现RCS的缩减,如B-2轰炸机,除了通过其扁平的外形设计实现雷达探测隐身外,在机体表面还涂覆4层RAM,以实现RCS缩减最大化,类似方式实现雷达隐身的还有F-22猛禽战机。但由于快速飞行目标的空气动力学因素限制,通过外形设计实现RCS缩减会引起目标机动性急剧下降,同时多层涂覆RAM会增加目标重量和厚度,另外能适用多波段的高吸收率RAM比较昂贵,使得其在目标隐身应用中的代价很高。有关资料表明,B-2和F-22每飞行一次需更换RAM,每次更换需35小时,成本花费高昂。鉴于外形和RAM隐身存在的诸多缺陷,研究人员开始探索更为经济有效的方法手段来实现目标隐身。With the rapid development of detection technology and electromagnetic stealth technology, stealth characteristics have gradually become an important indicator to measure the performance of flying targets. Reducing the target's Radar Cross Section (RCS) has become a key factor in preemptive strikes in modern warfare. Traditional stealth technology mainly reduces RCS by changing the shape of flying targets and coating radar absorbing materials (RAM). For example, the B-2 bomber, in addition to achieving radar detection stealth through its flat shape design, is also coated on the surface of the aircraft body. 4-layer RAM to maximize RCS reduction. The F-22 Raptor fighter also achieves radar stealth in a similar way. However, due to the aerodynamic limitations of fast-flying targets, reducing the RCS through shape design will cause a sharp decrease in the target's maneuverability. At the same time, multi-layer coating RAM will increase the weight and thickness of the target. In addition, the comparison of high-absorption RAMs that can be applied to multiple bands Expensive, making it costly in targeted stealth applications. Relevant information shows that the B-2 and F-22 need to replace the RAM every time they fly, and each replacement takes 35 hours, which is very costly. In view of the many shortcomings of appearance and RAM stealth, researchers began to explore more cost-effective methods to achieve target stealth.

人工磁导体(AMC)是一种由特定形状的单元结构按周期性排列而成的新型人工电磁材料,因其具有理想磁导体特性被应用于降低天线剖面、抑制表面波以及提高天线辐射性能等多种领域。其对反射波的相位调控能力有望能解决上述隐身方案中存在的缺陷,同时作为超材料的二维平面情形,容易与飞机、导弹等一些高速飞行目标共形,在军事、航天、通信系统中具有广阔应用前景。由于超表面的优异特性和强大电磁调控能力,其在目标电磁隐身中的潜在应用被逐渐发掘出来,并取得阶段性进展。2007年,棋盘结构的人工磁导体(AMC)超表面首次被应用于RCS缩减领域,虽然由于AMC-PEC组合的满足相消要求的频段较窄限制了它的实际应用,但该方法极大激发了人们对基于棋盘形式的新型宽带、极化不敏感、大角度入射的研究热潮,期望有朝一日这一技术能够真正用到实际中去,成为代替传统RAM的新型隐身材料。Artificial Magnetic Conductor (AMC) is a new type of artificial electromagnetic material composed of unit structures of specific shapes arranged periodically. Because of its ideal magnetic conductor properties, it is used to reduce antenna profiles, suppress surface waves, and improve antenna radiation performance. Various fields. Its phase control ability of reflected waves is expected to solve the shortcomings in the above-mentioned stealth solutions. At the same time, as a two-dimensional plane of metamaterials, it is easy to conform to some high-speed flying targets such as aircraft and missiles. It is widely used in military, aerospace, and communication systems. It has broad application prospects. Due to the excellent characteristics and powerful electromagnetic control capabilities of metasurfaces, their potential applications in target electromagnetic stealth have been gradually discovered and progress has been made in stages. In 2007, the artificial magnetic conductor (AMC) metasurface with a checkerboard structure was first used in the field of RCS reduction. Although the narrow frequency band of the AMC-PEC combination that meets the destructive requirements limits its practical application, this method has greatly inspired This has triggered an upsurge in research on new broadband, polarization-insensitive, and large-angle incidence devices based on the checkerboard pattern. It is hoped that one day this technology can be truly used in practice and become a new stealth material that replaces traditional RAM.

发明内容Contents of the invention

本发明所要解决的技术问题是针对背景技术中所涉及到的缺陷,提供一种基于缝隙加载的宽带RCS缩减超表面。The technical problem to be solved by the present invention is to provide a broadband RCS reduced metasurface based on gap loading in view of the defects involved in the background technology.

本发明为解决上述技术问题采用以下技术方案:The present invention adopts the following technical solutions to solve the above technical problems:

基于缝隙加载的宽带RCS缩减超表面,宽带RCS缩减超表面为二维有限尺寸结构,由第一AMC超单元、第二AMC超单元在平面内交错间隔阵列而成;Broadband RCS reduced metasurface based on gap loading. Broadband RCS reduced metasurface is a two-dimensional finite size structure, which is composed of the first AMC super unit and the second AMC super unit in a staggered spaced array in the plane;

所述第一AMC超单元、第二AMC超单元分别为由第一AMC单元、第二AMC单元按照3×3棋盘形式排列而成的正方形AMC超单元;The first AMC super unit and the second AMC super unit are respectively square AMC super units arranged in a 3×3 checkerboard format by the first AMC unit and the second AMC unit;

所述第一AMC单元、第二AMC单元呈大小相同的正方形,均包含上层金属结构、中层介质基板和下层金属地板;The first AMC unit and the second AMC unit are squares of the same size, and both include an upper metal structure, a middle dielectric substrate and a lower metal floor;

所述第一AMC单元的上层金属结构包含第一正方形贴片和第一正方框贴片,其中,第一正方框贴片套在所述第一正方形贴片外,两者的中心均和第一AMC单元中层介质基板的中心重合;第一正方形贴片、第一正方框贴片的两条对角线对应重合,且第一正方形贴片、第一正方框贴片均沿其两条对角线设有开槽,形成十字形开槽;所述第一正方框四条边的中心均设有小十字形开槽,所述小十字形开槽的一条开槽和其对应的边平行、另一条开槽和其对应的边垂直;The upper metal structure of the first AMC unit includes a first square patch and a first square frame patch, wherein the first square frame patch is placed outside the first square patch, and the centers of both are aligned with the first square patch. The centers of the middle dielectric substrates of an AMC unit coincide with each other; the two diagonal lines of the first square patch and the first square frame patch coincide with each other, and the first square patch and the first square frame patch are aligned along their two opposite sides. The corner lines are provided with slots to form cross-shaped slots; the centers of the four sides of the first square frame are provided with small cross-shaped slots, and one slot of the small cross-shaped slot is parallel to its corresponding side. The other slot is perpendicular to its corresponding side;

所述第二AMC单元的上层金属结构包含第二正方形贴片和第二正方框贴片,其中,第二正方框贴片套在所述第二正方形贴片外,两者的中心均和第二AMC单元中层介质基板的中心重合;第一正方形贴片、第一正方框贴片的两条对角线对应重合;The upper metal structure of the second AMC unit includes a second square patch and a second square frame patch, wherein the second square frame patch is placed outside the second square patch, and the centers of both are aligned with the second square patch. The centers of the middle dielectric substrates of the two AMC units coincide; the two diagonals of the first square patch and the first square frame patch overlap accordingly;

所述第一AMC单元、第二AMC单元均为对称反射结构,且第一AMC单元、第二AMC单元的上层金属结构的旋转角度相同,第一AMC单元、第二AMC单元的介质基板的厚度H的范围为0.01λ-0.1λ,λ为自由空间波长。The first AMC unit and the second AMC unit are both symmetrical reflective structures, and the rotation angles of the upper metal structures of the first AMC unit and the second AMC unit are the same. The thickness of the dielectric substrate of the first AMC unit and the second AMC unit is The range of H is 0.01λ-0.1λ, where λ is the free space wavelength.

作为本发明基于缝隙加载的宽带RCS缩减超表面进一步的优化方案,所述第一AMC单元、第二AMC单元的介质基板的介电常数er的范围为1-6,电损耗正切tanσ的范围为0.0005-0.02。As a further optimization solution for the broadband RCS reduction metasurface based on gap loading of the present invention, the dielectric constant er of the dielectric substrate of the first AMC unit and the second AMC unit ranges from 1 to 6, and the range of the electrical loss tangent tanσ is 0.0005-0.02.

作为本发明基于缝隙加载的宽带RCS缩减超表面进一步的优化方案,所述第一AMC单元、第二AMC单元的介质板厚度h为2.4mm、相对介电常数er=4.4;第一AMC单元、第二AMC单元的上层金属结构的厚度t=0.035mm。As a further optimization solution for the broadband RCS reduction metasurface based on gap loading of the present invention, the dielectric plate thickness h of the first AMC unit and the second AMC unit is 2.4mm, and the relative dielectric constant er=4.4; the first AMC unit, The thickness of the upper metal structure of the second AMC unit is t=0.035mm.

作为本发明基于缝隙加载的宽带RCS缩减超表面进一步的优化方案,所述第一正方框贴片中边的长度La=7mm、边的宽度Ws=1.5mm、平行于边的开槽的长度Ls=1mm;第一正方形贴片中边的长度Li=3mm;第二正方框贴片中边的长度a=5.6mm;第二正方形贴片中边的长度Lc=2.27mm;第二正方框贴片、第二正方形贴片的边之间的间距Wa=0.4mm,此时,第一AMC单元的谐振频点在12GHz;第二AMC单元为双频环型人工磁导体单元,谐振点分别为8.5GHz和17GHz。As a further optimization solution of the wideband RCS reduction metasurface based on gap loading of the present invention, the length of the side in the first square frame patch is La=7mm, the width of the side Ws=1.5mm, and the length of the slot parallel to the side Ls =1mm; the length of the middle side of the first square patch Li=3mm; the length of the middle side of the second square frame patch a=5.6mm; the length of the middle side of the second square patch Lc=2.27mm; the second square frame patch The distance Wa between the sides of the patch and the second square patch is 0.4mm. At this time, the resonant frequency point of the first AMC unit is 12GHz; the second AMC unit is a dual-frequency ring-type artificial magnetic conductor unit, and the resonance points are respectively 8.5GHz and 17GHz.

本发明采用以上技术方案与现有技术相比,具有以下技术效果:Compared with the existing technology, the present invention adopts the above technical solution and has the following technical effects:

1.结构简单,使用高效;1. Simple structure and efficient use;

2.解决了现有的基于人工磁导体棋盘结构形式的RCS减缩频段窄的问题;2. Solve the problem of narrow frequency band of the existing RCS based on artificial magnetic conductor checkerboard structure;

3.具有极化不敏感、缩减效果好等优异性能。3. It has excellent properties such as polarization insensitivity and good reduction effect.

附图说明Description of the drawings

图1为AMC-AMC棋盘形式电磁减缩超表面;Figure 1 shows the electromagnetic reduction metasurface in the form of AMC-AMC checkerboard;

图2(a)、(b)、(c)分别为第一AMC单元的俯视图、第一AMC单元的侧视图、第二AMC单元的俯视图;Figure 2(a), (b), and (c) are respectively a top view of the first AMC unit, a side view of the first AMC unit, and a top view of the second AMC unit;

图3为平面波垂直入射下的第一AMC单元等效电路图;Figure 3 is the equivalent circuit diagram of the first AMC unit under normal incidence of plane waves;

图4(a)、(b)、(c)、(d)、(e)分别为不加载缝隙时单元结构图、仅在正方框贴片上加载缝隙结构图、无内正方形贴片时加载缝隙单元结构图、不在内部正方形贴片上加载缝隙单元结构图、内外均加载缝隙的新型单元结构图;Figure 4(a), (b), (c), (d), and (e) are respectively the unit structure diagram when no gap is loaded, the gap structure diagram when only the square frame patch is loaded, and the unit structure diagram when there is no inner square patch. The structure diagram of the gap unit, the structure diagram of the unit without loading the gap on the internal square patch, and the structure diagram of the new unit with gaps loaded both inside and outside;

图5为图4(a)、(b)、(c)、(d)、(e)对应的各单元反射相位随频率变化曲线的对比图;Figure 5 is a comparison chart of the reflection phase versus frequency curves of each unit corresponding to Figure 4(a), (b), (c), (d), and (e);

图6为不同缝隙宽度n对单元反射相位的影响;Figure 6 shows the effect of different gap widths n on the reflection phase of the unit;

图7为AMC-PEC棋盘结构示意图;Figure 7 is a schematic diagram of the AMC-PEC chessboard structure;

图8(a)、(b)分别为单元反射相位随频率变化曲线、单元反射相位差随频率变化曲线;Figure 8(a) and (b) are respectively the unit reflection phase variation curve with frequency and the unit reflection phase difference variation curve with frequency;

图9(a)、(b)分别为9GHz下AMC-AMC电磁减缩超表面3D RCS散射图、9GHz下等尺寸金属板3D RCS散射图;Figure 9(a) and (b) are respectively the 3D RCS scattering diagram of the AMC-AMC electromagnetic reduced metasurface at 9GHz and the 3D RCS scattering diagram of the metal plate of equal size at 9GHz;

图10(a)、(b)分别为12GHz下AMC-AMC电磁减缩超表面3D RCS散射图、12GHz下等尺寸金属板3D RCS散射图;Figure 10(a) and (b) are respectively the 3D RCS scattering diagram of the AMC-AMC electromagnetic reduced metasurface at 12GHz and the 3D RCS scattering diagram of the metal plate of equal size at 12GHz;

图11为平面波垂直入射下AMC-AMC棋盘形式超表面RCS相对缩减量;Figure 11 shows the relative reduction in RCS of the AMC-AMC checkerboard metasurface under normal incidence of plane waves;

图12为不同角度下平面波入射AMC-AMC超表面RCS相对缩减量。Figure 12 shows the relative reduction in RCS of plane waves incident on the AMC-AMC metasurface at different angles.

具体实施方式Detailed ways

下面结合附图对本发明的技术方案做进一步的详细说明:The technical solution of the present invention will be further described in detail below in conjunction with the accompanying drawings:

本发明可以以许多不同的形式实现,而不应当认为限于这里所述的实施例。相反,提供这些实施例以便使本公开透彻且完整,并且将向本领域技术人员充分表达本发明的范围。在附图中,为了清楚起见放大了组件。The invention may be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the scope of the invention to those skilled in the art. In the drawings, components are exaggerated for clarity.

如图1所示,宽带RCS缩减超表面为二维有限尺寸结构,由第一AMC超单元、第二AMC超单元在平面内交错间隔阵列而成;As shown in Figure 1, the broadband RCS reduced metasurface is a two-dimensional finite size structure, which is composed of the first AMC super unit and the second AMC super unit in a staggered spaced array in the plane;

所述第一AMC超单元、第二AMC超单元分别为由第一AMC单元、第二AMC单元按照3×3棋盘形式排列而成的正方形AMC超单元;The first AMC super unit and the second AMC super unit are respectively square AMC super units arranged in a 3×3 checkerboard format by the first AMC unit and the second AMC unit;

所述第一AMC单元、第二AMC单元呈大小相同的正方形,均包含上层金属结构、中层介质基板和下层金属地板;The first AMC unit and the second AMC unit are squares of the same size, and both include an upper metal structure, a middle dielectric substrate and a lower metal floor;

所述第一AMC单元的上层金属结构包含第一正方形贴片和第一正方框贴片,其中,第一正方框贴片套在所述第一正方形贴片外,两者的中心均和第一AMC单元中层介质基板的中心重合;第一正方形贴片、第一正方框贴片的两条对角线对应重合,且第一正方形贴片、第一正方框贴片均沿其两条对角线设有开槽,形成十字形开槽;所述第一正方框四条边的中心均设有小十字形开槽,所述小十字形开槽的一条开槽和其对应的边平行、另一条开槽和其对应的边垂直;The upper metal structure of the first AMC unit includes a first square patch and a first square frame patch, wherein the first square frame patch is placed outside the first square patch, and the centers of both are aligned with the first square patch. The centers of the middle dielectric substrates of an AMC unit coincide with each other; the two diagonal lines of the first square patch and the first square frame patch coincide with each other, and the first square patch and the first square frame patch are aligned along their two opposite sides. The corner lines are provided with slots to form cross-shaped slots; the centers of the four sides of the first square frame are provided with small cross-shaped slots, and one slot of the small cross-shaped slot is parallel to its corresponding side. The other slot is perpendicular to its corresponding side;

所述第二AMC单元的上层金属结构包含第二正方形贴片和第二正方框贴片,其中,第二正方框贴片套在所述第二正方形贴片外,两者的中心均和第二AMC单元中层介质基板的中心重合;第一正方形贴片、第一正方框贴片的两条对角线对应重合;The upper metal structure of the second AMC unit includes a second square patch and a second square frame patch, wherein the second square frame patch is placed outside the second square patch, and the centers of both are aligned with the second square patch. The centers of the middle dielectric substrates of the two AMC units coincide; the two diagonals of the first square patch and the first square frame patch overlap accordingly;

所述第一AMC单元、第二AMC单元均为对称反射结构,且第一AMC单元、第二AMC单元的上层金属结构的旋转角度相同,第一AMC单元、第二AMC单元的介质基板的厚度H的范围为0.01λ-0.1λ,λ为自由空间波长。The first AMC unit and the second AMC unit are both symmetrical reflective structures, and the rotation angles of the upper metal structures of the first AMC unit and the second AMC unit are the same. The thickness of the dielectric substrate of the first AMC unit and the second AMC unit is The range of H is 0.01λ-0.1λ, where λ is the free space wavelength.

所述第一AMC超单元、第二AMC超单元之间的反射相位差在9-18GHz范围内满足143°-217°之间。The reflection phase difference between the first AMC super unit and the second AMC super unit satisfies a range of 143°-217° in the range of 9-18 GHz.

所述第一AMC单元、第二AMC单元的介质基板的介电常数er的范围为1-6,电损耗正切tanσ的范围为0.0005-0.02。The dielectric constant er of the dielectric substrate of the first AMC unit and the second AMC unit ranges from 1 to 6, and the electrical loss tangent tanσ ranges from 0.0005 to 0.02.

所述第一AMC单元、第二AMC单元的介质板厚度h为2.4mm、相对介电常数er=4.4;第一AMC单元、第二AMC单元的上层金属结构的厚度t=0.035mm,所述第一正方框贴片中边的长度La=7mm、边的宽度Ws=1.5mm、平行于边的开槽的长度Ls=1mm;第一正方形贴片中边的长度Li=3mm;第二正方框贴片中边的长度a=5.6mm;第二正方形贴片中边的长度Lc=2.27mm;第二正方框贴片、第二正方形贴片的边之间的间距Wa=0.4mm,此时,第一AMC单元的谐振频点在12GHz;第二AMC单元为双频环型人工磁导体单元,谐振点分别为8.5GHz和17GHz。The thickness h of the dielectric plate of the first AMC unit and the second AMC unit is 2.4mm, and the relative dielectric constant er=4.4; the thickness t of the upper metal structure of the first AMC unit and the second AMC unit is 0.035mm. The length of the side in the first square frame patch is La=7mm, the width of the side is Ws=1.5mm, and the length of the slot parallel to the side is Ls=1mm; the length of the side in the first square patch is Li=3mm; the length of the side in the second square patch is Li=3mm. The length of the middle side of the frame patch a = 5.6mm; the length of the middle side of the second square patch Lc = 2.27mm; the distance between the sides of the second square frame patch and the second square patch Wa = 0.4mm, this At , the resonant frequency point of the first AMC unit is 12GHz; the second AMC unit is a dual-frequency ring-type artificial magnetic conductor unit, and the resonant points are 8.5GHz and 17GHz respectively.

为了方便表述,下面将第一AMC单元记为AMC 1、第二AMC单元记为AMC 2,将第一正方框贴片、第一正方形贴片中各个开槽的宽度记为n。For convenience of description, the first AMC unit is denoted as AMC 1 and the second AMC unit is denoted as AMC 2, and the width of each slot in the first square frame patch and the first square patch is denoted as n.

本发明的设计方法步骤,主要有以下三步设计流程:The design method steps of the present invention mainly include the following three-step design process:

第一步:基于缝隙加载的新型宽带、极化不敏感AMC单元设计:Step one: Design of a new broadband, polarization-insensitive AMC unit based on gap loading:

依据棋盘形式的宽带、极化不敏感RCS减缩超表面设计,首要问题是设计具有宽频工作和极化不敏感特性的AMC单元,其基本理论依据是利用阵列理论中的反射相消原理,利用AMC单元反射相位随频率变化的特性使得相邻阵元间的反射相位差在宽频范围内满足143°-217°,实现反射波的能量相消从而达到后向RCS缩减。根据极化转化相关领域知识,要想获得极化不敏感特性,单元必须具有四周旋转对称特性。同时为获得宽频特性,则相位响应在很宽频率范围内具有线性度好、品质因数低等优异特性。Based on the broadband, polarization-insensitive RCS reduced metasurface design in the form of a checkerboard, the primary issue is to design an AMC unit with broadband operation and polarization-insensitive characteristics. The basic theoretical basis is to use the reflection destructive principle in array theory. The characteristic of the unit reflection phase changing with frequency makes the reflection phase difference between adjacent array elements satisfy 143°-217° in a wide frequency range, realizing the energy cancellation of the reflected wave and achieving backward RCS reduction. According to knowledge related to polarization conversion, in order to obtain polarization insensitivity, the unit must have four-week rotational symmetry. At the same time, in order to obtain broadband characteristics, the phase response has excellent characteristics such as good linearity and low quality factor in a wide frequency range.

根据上述分析,我们发明了一种基于多对十字形缝隙加载的新型宽带人工磁导体单元结构,图2(a)、(b)、(c)分别为第一AMC单元的俯视图、第二AMC单元的俯视图、第一AMC单元的侧视图。AMC 1由上层金属结构、中层介质板和底层金属地板组成,由于上层金属结构加载了多条缝隙后使得自身的等效电感和电容特性被激发,因此成为了强谐振结构,利用等效电路原理可知,单元相位的线性度和加载的缝隙有着至关重要的联系,通过在外环上加载缝隙增加了电磁波入射下激励的电流流动增加了电感L,在内环上加载两条长缝隙增加了串联电容使得C减小,从而最终达到拓展单元工作带宽的目的,图3为AMC1在平面波垂直入射下的等效电路图。Based on the above analysis, we invented a new broadband artificial magnetic conductor unit structure based on multiple pairs of cross-shaped gap loading. Figure 2(a), (b), and (c) are the top view of the first AMC unit and the second AMC unit respectively. Top view of the unit, side view of the first AMC unit. AMC 1 is composed of an upper metal structure, a middle dielectric board and a bottom metal floor. Since the upper metal structure is loaded with multiple gaps, its equivalent inductance and capacitance characteristics are excited, so it becomes a strong resonance structure, using the equivalent circuit principle. It can be seen that The linearity of the unit phase is crucially related to the loaded gap. By loading the gap on the outer ring, the current flow excited by the incident electromagnetic wave increases and the inductance L is increased. Loading two long gaps on the inner ring increases the series capacitance. This reduces C, thereby ultimately achieving the purpose of expanding the operating bandwidth of the unit. Figure 3 is the equivalent circuit diagram of AMC1 under vertical incidence of plane waves.

为了清楚地展示单元上加载的缝隙对同相反射频带的影响,图4(a)为不加载缝隙时单元结构图、(b)为在正方框贴片上加载缝隙单元结构图、(c)为无内正方形贴片时加载缝隙单元结构图、(d)为不在内部正方形贴片上加载缝隙单元结构图、(e)为内外均加载缝隙的新型单元结构图,图5给出了加载外部缝隙、加载内部缝隙以及内外均加载缝隙后对单元反射相位的影响。可以看出外环加载缝隙对单元的带宽影响较大,同时加载多对缝隙之后使得单元的同相反射频带得到有效提升。In order to clearly show the impact of the gap loaded on the unit on the in-phase reflection frequency band, Figure 4(a) shows the structure diagram of the unit without loading the gap, (b) shows the structure diagram of the unit loading the slot on the square frame patch, (c) (d) is the structure diagram of the unit loaded with gaps when there is no inner square patch, (d) is the structure diagram of the unit without loading gaps on the inner square patch, (e) is the structural diagram of the new unit with gaps loaded both inside and outside, Figure 5 shows the structure diagram of loading the outside The effect on the reflection phase of the unit after loading gaps, loading internal gaps, and loading gaps both inside and outside. It can be seen that loading the slots in the outer ring has a greater impact on the bandwidth of the unit. Loading multiple pairs of slots at the same time effectively improves the in-phase reflection frequency band of the unit.

为进一步解释本结构宽带特性的原因,图6给出了中间加载的一对十字型缝隙宽度n不同尺寸下的反射相位影响,可以看出增加n时,AMC1的谐振点向高频偏移,同时拓展了单元的同相反射频带。In order to further explain the reasons for the broadband characteristics of this structure, Figure 6 shows the impact of the reflection phase under different sizes of a pair of cross-shaped gap widths n loaded in the middle. It can be seen that when n is increased, the resonance point of AMC1 shifts to high frequency. At the same time, the in-phase reflection frequency band of the unit is expanded.

同时由于单元具有旋转对称特性,不同极化电磁波照射到AMC单元时会产生相似的谐振效果,单元电磁散射响应对x、y线极化波具有极化不敏感性,为构建极化不敏感的低RCS电磁表面提供了合适的结构。At the same time, due to the rotational symmetry of the unit, similar resonance effects will occur when electromagnetic waves of different polarizations are irradiated to the AMC unit. The electromagnetic scattering response of the unit is polarization insensitive to x- and y-line polarization waves, which is a good way to build a polarization-insensitive Low RCS electromagnetic surface provides suitable structure.

为使单元相位特性达到最宽,利用商业仿真软件CST对单元结构参数进行优化。最终单元周期为p=10mm,介质板为厚度为2.4mm、相对介电常数4.4、电损耗正切0.02的聚四氟乙烯,底层金属铜板厚度可为0.035mm。通过改变整个金属结构尺寸a而保持其他参数不变来获得想要的相位分布。最终AMC单元1尺寸为t=0.035mm,AMC1中La=7mm,Ls=1mm,Ws=1.5mm,Li=3mm。In order to maximize the unit phase characteristics, commercial simulation software CST is used to optimize the unit structure parameters. The final unit period is p=10mm, the dielectric plate is polytetrafluoroethylene with a thickness of 2.4mm, a relative dielectric constant of 4.4, and an electrical loss tangent of 0.02. The thickness of the underlying metal copper plate can be 0.035mm. The desired phase distribution is obtained by changing the overall metal structure dimension a while keeping other parameters unchanged. The final size of AMC unit 1 is t=0.035mm, La=7mm, Ls=1mm, Ws=1.5mm, Li=3mm in AMC1.

第二步:基于阵列理论的双频环型AMC单元设计:Step 2: Design of dual-frequency ring-type AMC unit based on array theory:

AMC-AMC棋盘形式结构是经过AMC-PEC形式改进得来的,但是两种形式的分析原理是一样的,通常采用阵列理论进行分析。下面对AMC-PEC棋盘形式缩减后向RCS原理进行分析,如图4所示,根据阵列理论可知,当电磁波垂直入射时,由于AMC结构和PEC结构均为全反射结构,所以两种结构的反射幅度一致,总的反射电场可以由下面公式表示:The AMC-AMC checkerboard form structure is improved from the AMC-PEC form, but the analysis principles of the two forms are the same, and array theory is usually used for analysis. The following is an analysis of the AMC-PEC checkerboard form reduced backward RCS principle, as shown in Figure 4. According to the array theory, when electromagnetic waves are vertically incident, since both the AMC structure and the PEC structure are total reflection structures, the The reflection amplitude is consistent, and the total reflected electric field can be expressed by the following formula:

E=EAMC·AFAMC+EPEC·AFPEC (1)E=E AMC ·AF AMC +E PEC ·AF PEC (1)

其中AMC和PEC块反射的电场分量可表示为:The electric field components reflected by the AMC and PEC blocks can be expressed as:

其中Φ1、Φ2分别表示AMC和PEC的反射相位,AFAMC、AFPEC分别是AMC结构和PEC结构的阵列因子,并且由于两种结构的反射幅度相同,所以可以得到Among them, Φ1 and Φ2 represent the reflection phases of AMC and PEC respectively, AFAMC and AFPEC are the array factors of the AMC structure and PEC structure respectively, and since the reflection amplitudes of the two structures are the same, we can get

阵列因子表示为The array factor is expressed as

式中,d为AMC结构与PEC结构的中心间距,并且In the formula, d is the center distance between the AMC structure and the PEC structure, and

可以看出,当电磁波垂直入射,即入射角度为0时,可以得到,所以可已得到总的辐射场为It can be seen that when the electromagnetic wave is vertically incident, that is, when the incident angle is 0, it can be obtained, so the total radiation field can be obtained as

当法线方向上的反射波能量比入射波能量小10dB以上时,即When the reflected wave energy in the normal direction is more than 10dB smaller than the incident wave energy, that is

|E|2/|E0|2≤-10dB (7)|E| 2 /|E 0 | 2 ≤-10dB (7)

进一步计算可以得到Further calculation can be obtained

上式揭示了PEC和AMC的相位与RCS缩减量的关系,因为PEC的反射相位为固定的180度,所以可以得到AMC的相位条件The above equation reveals the relationship between the phases of PEC and AMC and the amount of RCS reduction. Because the reflection phase of PEC is fixed at 180 degrees, the phase condition of AMC can be obtained.

当满足上述条件时,AMC-PEC棋盘结构的后向RCS缩减可以达到10dB。可以看出对于一般的单元来说,单元结构的相位处于上述条件之间的带宽较窄,限制了RCS缩减的带宽。研究人员利用另一种AMC结构来代替PEC结构,使得两种结构都处于可调的状态,当满足相位差条件时实现RCS缩减,大大提高了缩减带宽,公式计算得到相位差条件为When the above conditions are met, the backward RCS reduction of the AMC-PEC checkerboard structure can reach 10dB. It can be seen that for general units, the bandwidth of the phase of the unit structure between the above conditions is narrow, which limits the bandwidth of RCS reduction. The researchers used another AMC structure to replace the PEC structure, so that both structures are in an adjustable state. When the phase difference condition is met, RCS reduction is achieved, which greatly improves the reduction bandwidth. The phase difference condition calculated by the formula is

当满足上述条件时,由于AMC-AMC棋盘结构的两个部分反射幅度相等,相位相差180度,所以反射方向的能量被散射到其他方向,即在反射方向上反射波由一束主波束变换为多波束形式,这样可以在该方向上实现RCS缩减。若可以将宽带AMC单元结合具有双谐振点的AMC单元,使得宽带AMC单元的谐振点位于双频AMC单元的两个谐振点中间则可以最大程度上利用反射相位差满足10dB的RCS减缩条件。据此设计了一种双频段环型谐振AMC单元2,通过合理调节双环型AMC2中的内外尺寸,使得AMC2分别在8.5GHz和17GHz处发生谐振,两种不同单元的反射相位特性和相位差随频率变化曲线如图8(a)、(b)所示,最终AMC2中的尺寸为a=5.6mm,Lc=2.27mm,Wa=0.4mm,并实现了在9~18GHz频段内,AMC1单元和AMC2单元之间的反射相位差保持在150°~210°之间,即理想情况下在此频段内的RCS缩减量可达10dB以上。When the above conditions are met, since the reflection amplitude of the two parts of the AMC-AMC checkerboard structure is equal and the phase difference is 180 degrees, the energy in the reflection direction is scattered to other directions, that is, the reflected wave in the reflection direction is transformed from a main beam to Multi-beam form, which can achieve RCS reduction in this direction. If the broadband AMC unit can be combined with an AMC unit with dual resonance points, so that the resonance point of the broadband AMC unit is located between the two resonance points of the dual-frequency AMC unit, the reflection phase difference can be maximized to meet the 10dB RCS reduction condition. Based on this, a dual-band ring-type resonant AMC unit 2 is designed. By reasonably adjusting the internal and external dimensions of the double-ring AMC2, AMC2 resonates at 8.5GHz and 17GHz respectively. The reflection phase characteristics and phase difference of the two different units vary with the The frequency change curves are shown in Figure 8(a) and (b). The final dimensions of AMC2 are a=5.6mm, Lc=2.27mm, Wa=0.4mm, and the AMC1 unit and The reflection phase difference between AMC2 units is maintained between 150° and 210°, that is, ideally, the RCS reduction in this frequency band can reach more than 10dB.

第三步:基于第一步的新型宽带AMC单元设计和第二步的2种满足相位差要求的AMC单元设计,第三步则是如何合理利用2种AMC单元构建RCS减缩超表面。首先需要确定超表面的尺寸,也即超单元的数量。这里为便于设计,超表面采用方形布局,即x、y方向的AMC单元数量L和M相同。综合衡量计算时间、样品制作成本与超表面有限尺寸对RCS减缩特性的影响,这里超表面中AMC单元的数量为L×M=9×9,尺寸为90×90mm2;The third step: Based on the design of a new broadband AMC unit in the first step and the design of two AMC units that meet the phase difference requirements in the second step, the third step is how to rationally utilize the two AMC units to construct an RCS reduced metasurface. First, we need to determine the size of the metasurface, that is, the number of superunits. To facilitate design here, the metasurface adopts a square layout, that is, the number L and M of AMC units in the x and y directions are the same. To comprehensively measure the impact of calculation time, sample production cost and the limited size of the metasurface on the RCS reduction characteristics, the number of AMC units in the metasurface is L×M=9×9, and the size is 90×90mm2;

其次确定2种AMC单元的排列方式。为最大程度上打散入射电磁波,减小目标在各给角度上的散射强度从而降低单站RCS检测下的雷达发现几率,超表面中的单元排布形式有传统方形和间隔排列形,而间隔排列的形式又分AMC块1和块2间隔排列及AMC单元1和单元2间隔排列两种情况。由于实际电磁表面的有限性因此需要通过电磁仿真软件对其进行具体优化,最终本发明设计了一种由3×3棋盘形式的电磁隐身表面,具体排布顺序为222-111-,“-”表示AMC单元转折处,数字代表对应的不同AMC单元,与图1中数字序列对应。最终AMC-AMC分布如图1中所示,通过这种排列方式设计的超表面保证了任意相邻AMC单元在保证继承无限大排布的情况下的相位差分布,从而可以最大限度破坏超表面一致散射的等相位面,达到最大限度打散电磁波的目的。Next, determine the arrangement of the two AMC units. In order to disperse the incident electromagnetic waves to the greatest extent, reduce the scattering intensity of the target at various angles, and thus reduce the probability of radar discovery under single-station RCS detection, the unit arrangement in the metasurface includes traditional square and spaced arrangements, and spaced The arrangement forms are divided into two situations: AMC block 1 and block 2 are arranged at intervals, and AMC unit 1 and unit 2 are arranged at intervals. Due to the limitations of the actual electromagnetic surface, it needs to be specifically optimized through electromagnetic simulation software. Finally, the present invention designed an electromagnetic stealth surface in the form of a 3×3 checkerboard. The specific arrangement sequence is 222-111-, "-" Indicates the turning point of the AMC unit, and the numbers represent the corresponding different AMC units, which correspond to the numerical sequence in Figure 1. The final AMC-AMC distribution is shown in Figure 1. The metasurface designed through this arrangement ensures the phase difference distribution of any adjacent AMC unit while ensuring the inheritance of an infinite arrangement, thereby maximizing the destruction of the metasurface. Uniform scattering of equal-phase planes achieves the purpose of maximizing the scattering of electromagnetic waves.

最后根据AMC单元1和AMC单元2以3×3为一个局部单元间隔循环排列方式,在CST中建立棋盘形式超表面结构。Finally, according to the cyclic arrangement of AMC unit 1 and AMC unit 2 with a local unit interval of 3×3, a checkerboard-shaped metasurface structure is established in CST.

下面以3×3个AMC单元通过间隔排列构成的棋盘形式超表面为例,介绍设计过程,设计结果,并对结果进行分析。为揭示本发明方法的优越性,将其结果与等尺寸理想金属板的散射特性进行对比。为公平比较,两种情形下表面尺寸、介质板规格、入射角度等条件完全相同。The following takes a checkerboard-shaped metasurface composed of 3×3 AMC units arranged at intervals as an example to introduce the design process, design results, and analyze the results. In order to reveal the superiority of the method of the present invention, the results are compared with the scattering characteristics of an ideal metal plate of equal size. For fair comparison, the surface dimensions, dielectric plate specifications, incident angle and other conditions are exactly the same in the two cases.

仿真设计中,介质板采用聚四氟乙烯,其介电常数εr=4.4,电正切损耗tanσ=0.02,金属铜箔厚度0.035mm,介质板厚度为h=2.4mm,两种AMC单元周期均为p=10mm,构成棋盘形式的两种AMC单元的几何结构参数分别为:AMC1中La=7mm,Ls=1mm,Ws=1.5mm,Li=3mm;AMC2中a=5.6mm,Lc=2.27mm,Wa=0.4mm。In the simulation design, the dielectric board uses polytetrafluoroethylene, its dielectric constant εr = 4.4, the electrical tangent loss tanσ = 0.02, the metal copper foil thickness is 0.035mm, the dielectric board thickness is h = 2.4mm, and the two AMC unit periods are p=10mm, the geometric structure parameters of the two AMC units that form a checkerboard are: La=7mm, Ls=1mm, Ws=1.5mm, Li=3mm in AMC1; a=5.6mm, Lc=2.27mm in AMC2, Wa=0.4mm.

AMC单元的工作原理:当电磁波垂直入射时,y、x极化电场作用下会在平行于极化方向上的金属细贴片上产生感应电流,而上层金属结构由于加载了多对缝隙后使得相邻金属之间引入了等效电容,单元自身发生了强谐振因此相邻单元之间的耦合程度变得微弱,更好地模拟无限单元的情况。由于单元具有旋转对称性以及棋盘形式固有的对称性,因此y、x两种极化下具有完全相同的电磁响应,同时为了减小单元之间的间距使得结构更加紧凑,两种单元均围绕中心旋转45°。The working principle of the AMC unit: When the electromagnetic wave is vertically incident, the y and x polarized electric fields will generate an induced current on the thin metal patch parallel to the polarization direction, and the upper metal structure is loaded with multiple pairs of gaps. Equivalent capacitance is introduced between adjacent metals, and the unit itself undergoes strong resonance, so the degree of coupling between adjacent units becomes weak, better simulating the situation of infinite units. Since the unit has rotational symmetry and the inherent symmetry of the checkerboard form, it has exactly the same electromagnetic response under both y and x polarizations. At the same time, in order to reduce the distance between the units and make the structure more compact, both units are centered around the center. Rotate 45°.

AMC-AMC棋盘形式超表面RCS缩减原理:一方面,2种AMC单元的反射相位各异,当平面波垂直照射到由设计的两种AMC单元构成的超表面上时,根据阵列理论可知,反射波会被这些具有不同反射相位的AMC单元打散,因此实现了原方向上的电磁隐身。AMC-AMC checkerboard form metasurface RCS reduction principle: On the one hand, the reflection phases of the two types of AMC units are different. When the plane wave is vertically irradiated onto the metasurface composed of the two designed AMC units, according to the array theory, it can be seen that the reflected wave will be scattered by these AMC units with different reflection phases, thus achieving electromagnetic stealth in the original direction.

通过优化调整单元的金属结构参数和加载的缝隙尺寸可以控制AMC单元的谐振点以及同相反射带宽从而调谐整个单元的反射相位,获得最佳线性度和宽带相位响应。By optimally adjusting the metal structure parameters of the unit and the loaded gap size, the resonance point and in-phase reflection bandwidth of the AMC unit can be controlled to tune the reflection phase of the entire unit to obtain the best linearity and broadband phase response.

为验证本发明基于AMC-AMC棋盘形式超表面的宽带散射特性,采用商业仿真软件CST Microwave Studio对超表面的散射频谱进行电磁仿真,其中沿x、y、z方向的6个边界均采用开放边界条件,平面波沿-z方向垂直入射,采用平面线极化波进行垂直照射。In order to verify the broadband scattering characteristics of the AMC-AMC chessboard-shaped metasurface of the present invention, the commercial simulation software CST Microwave Studio was used to conduct electromagnetic simulation of the scattering spectrum of the metasurface, in which the six boundaries along the x, y, and z directions were all open boundaries. Conditions, plane waves are vertically incident along the -z direction, and plane linearly polarized waves are used for vertical illumination.

实施例尺寸为90mm×90mm×2.4mm的AMC-AMC棋盘形式超表面的宽带RCS减缩结果。Example: Broadband RCS reduction results of an AMC-AMC checkerboard metasurface with dimensions of 90 mm × 90 mm × 2.4 mm.

下面对上式设计的超表面RCS减缩结果进行说明和验证。由于棋盘形式和两种AMC本身固有的对称性可知,该电磁隐身表面具有极化不敏感特性,棋盘形式超表面均能很好地降低后向RCS,具有几乎完全相同的散射频谱响应,验证了本发明超表面的极化不敏感特性。同时,RCS减缩频谱结果显示棋盘形式超表面在8-20GHz范围内具有优异的RCS缩减特性,其中RCS减缩值均超过7.5dB的有效带宽为9-19GHz。The metasurface RCS reduction results of the above-mentioned design are explained and verified below. Due to the checkerboard form and the inherent symmetry of the two AMCs, it can be seen that the electromagnetic stealth surface has polarization insensitivity characteristics. Both checkerboard form metasurfaces can reduce the backward RCS well and have almost identical scattering spectrum responses, which is verified. Polarization-insensitive properties of the metasurface of the present invention. At the same time, the RCS reduction spectrum results show that the checkerboard-shaped metasurface has excellent RCS reduction characteristics in the range of 8-20GHz, in which the RCS reduction values exceed 7.5dB and the effective bandwidth is 9-19GHz.

为验证超表面的双站RCS减缩特性,对远区散射场进行仿真,得到超表面的3D散射方向图。图9(a)、图9(b)分别给出了等尺寸理想金属板在9GHz、12GHz处的远区3D散射方向图,图10(a)、图10(b)分别给出了双频段AMC-AMC超表面在9GHz、12GHz处的远区3D散射方向图。可以看出,与金属板的镜像强散射相比,AMC-AMC棋盘形式超表面能完美地将反射电磁波均匀打散在四个方向上,原方向上的散射能量被分散到了四个方向从而降低了来波垂直照射下表面的RCS。In order to verify the two-station RCS reduction characteristics of the metasurface, the far-area scattering field was simulated to obtain the 3D scattering pattern of the metasurface. Figure 9(a) and Figure 9(b) respectively show the far-zone 3D scattering pattern of an ideal metal plate of equal size at 9GHz and 12GHz. Figure 10(a) and Figure 10(b) respectively show the dual frequency band Far-zone 3D scattering pattern of AMC-AMC metasurface at 9GHz and 12GHz. It can be seen that compared with the strong mirror scattering of the metal plate, the AMC-AMC checkerboard-shaped metasurface can perfectly disperse the reflected electromagnetic waves evenly in four directions. The scattering energy in the original direction is dispersed in the four directions, thus reducing the The incoming wave vertically illuminates the RCS on the lower surface.

为进一步验证本发明方法打散电磁波和实现超宽带RCS缩减的能力,改变电磁波的入射角度可以看出15°、30°和45°入射情形下仿真结果表明,在电磁波入射角度小于45°范围内的所有情形下,超表面均能在12.5-17.5GHz内很好实现7.5dB以上的RCS缩减效果。当入射角为0°时,AMC-AMC棋盘形式超表面的7.5dB RCS缩减仿真带宽为8-19.2GHz;入射角为15°时,7.5dB RCS缩减仿真带宽为8-18.5GHz;入射角为30°时,7.5dB RCS缩减仿真带宽为11-17.8GHz;入射角为45°时,RCS减缩性能有所下降,但均满足7.5dB以上的RCS缩减效果且R仿真带宽达12.5-17.5GHz,综上所述,棋盘形式AMC-AMC超表面在大角度(最高可达45°)入射情况下,在9-18GHz内依然具有很好的RCS缩减特性。In order to further verify the ability of the method of the present invention to disperse electromagnetic waves and achieve ultra-wideband RCS reduction, changing the incident angle of electromagnetic waves shows that the simulation results under the incident situations of 15°, 30° and 45° show that when the incident angle of electromagnetic waves is less than 45°, In all cases, the metasurface can achieve an RCS reduction effect of more than 7.5dB within 12.5-17.5GHz. When the incident angle is 0°, the 7.5dB RCS reduced simulation bandwidth of the AMC-AMC checkerboard metasurface is 8-19.2GHz; when the incident angle is 15°, the 7.5dB RCS reduced simulation bandwidth is 8-18.5GHz; the incident angle is At 30°, the 7.5dB RCS reduction simulation bandwidth is 11-17.8GHz; when the incident angle is 45°, the RCS reduction performance decreases, but both meet the RCS reduction effect of more than 7.5dB and the R simulation bandwidth reaches 12.5-17.5GHz. To sum up, the checkerboard-shaped AMC-AMC metasurface still has good RCS reduction characteristics in the range of 9-18GHz under the condition of large angle (up to 45°) incidence.

图11和图12给出了电磁波垂直入射时和不同角度入射时的RCS缩减结果。Figures 11 and 12 show the RCS reduction results when electromagnetic waves are incident vertically and at different angles.

综上,近场分布、远场散射方向图与RCS减缩频谱均显示基于AMC-AMC棋盘形式的超表面的超宽带、极化不敏感RCS减缩特性和均匀打散电磁波能力,上述特性和能力在45°的入射角范围下依旧保持的很好。该超表面设计简单、效果明显、对极化和入射角具有很好的鲁棒性、无需优化,具有固有打散电磁波的能力,同时所提出的基于缝隙加载的宽带人工磁导体结构同相反射频带较宽、单元之间耦合影响小,本发明设计的电磁隐身表面和新型人工磁导体结构在未来电磁隐身领域以及天线小型化设计中具有重要潜在应用价值。In summary, the near-field distribution, far-field scattering pattern and RCS reduction spectrum all show the ultra-wideband, polarization-insensitive RCS reduction characteristics and ability to uniformly disperse electromagnetic waves based on the AMC-AMC checkerboard metasurface. The above characteristics and capabilities are in It still maintains very good performance under the incident angle range of 45°. The metasurface is simple in design, has obvious effects, is very robust to polarization and incident angle, does not require optimization, and has the inherent ability to disperse electromagnetic waves. At the same time, the proposed broadband artificial magnetic conductor structure based on gap loading has in-phase reflection frequency. The band is wider and the coupling effect between units is small. The electromagnetic stealth surface and new artificial magnetic conductor structure designed in the present invention have important potential application value in the future electromagnetic stealth field and antenna miniaturization design.

本技术领域技术人员可以理解的是,除非另外定义,这里使用的所有术语(包括技术术语和科学术语)具有与本发明所属领域中的普通技术人员的一般理解相同的意义。还应该理解的是,诸如通用字典中定义的那些术语应该被理解为具有与现有技术的上下文中的意义一致的意义,并且除非像这里一样定义,不会用理想化或过于正式的含义来解释。It can be understood by one of ordinary skill in the art that, unless otherwise defined, all terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this invention belongs. It should also be understood that terms such as those defined in general dictionaries are to be understood to have meanings consistent with their meaning in the context of the prior art, and are not to be taken in an idealized or overly formal sense unless defined as herein. explain.

以上所述的具体实施方式,对本发明的目的、技术方案和有益效果进行了进一步详细说明,所应理解的是,以上所述仅为本发明的具体实施方式而已,并不用于限制本发明,凡在本发明的精神和原则之内,所做的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The above-mentioned specific embodiments further describe the objectives, technical solutions and beneficial effects of the present invention in detail. It should be understood that the above-mentioned are only specific embodiments of the present invention and are not intended to limit the present invention. Any modifications, equivalent substitutions, improvements, etc. made within the spirit and principles of the present invention shall be included in the protection scope of the present invention.

Claims (4)

1. The broadband RCS reduction super surface based on gap loading is characterized in that the broadband RCS reduction super surface is of a two-dimensional limited-size structure and is formed by staggered interval arrays of a first AMC super unit and a second AMC super unit in a plane;
the first AMC superunit and the second AMC superunit are square AMC superunits formed by arranging the first AMC unit and the second AMC unit in a 3 multiplied by 3 chessboard mode respectively;
the first AMC units and the second AMC units are square with the same size and each comprise an upper metal structure, a middle dielectric substrate and a lower metal floor;
the upper metal structure of the first AMC unit comprises a first square patch and a first square frame patch, wherein the first square frame patch is sleeved outside the first square patch, and the centers of the first square frame patch and the first square frame patch are overlapped with the center of the middle layer dielectric substrate of the first AMC unit; the two diagonal lines of the first square patch and the first square frame patch are correspondingly overlapped, and grooves are formed in the first square patch and the first square frame patch along the two diagonal lines of the first square patch and the first square frame patch respectively to form cross grooves; the centers of the four sides of the first positive square frame are respectively provided with a small cross slot, one slot of the small cross slot is parallel to the corresponding side of the small cross slot, and the other slot is perpendicular to the corresponding side of the small cross slot;
the upper metal structure of the second AMC unit comprises a second square patch and a second square frame patch, wherein the second square frame patch is sleeved outside the second square patch, and the centers of the second square frame patch and the second square frame patch are overlapped with the center of the middle layer dielectric substrate of the second AMC unit; the two diagonal lines of the first square patch and the first square frame patch are correspondingly overlapped;
the first AMC unit and the second AMC unit are both symmetrical reflection structures, the rotation angles of the upper metal structures of the first AMC unit and the second AMC unit are the same, the thickness h of the dielectric substrates of the first AMC unit and the second AMC unit ranges from 0.01λ to 0.1λ, and λ is the free space wavelength.
2. The gap-loading based broadband RCS reduced super surface according to claim 1, wherein the dielectric substrates of the first and second AMC units have a dielectric constant er ranging from 1 to 6 and an electric loss tangent tan σ ranging from 0.0005 to 0.02.
3. The slot loading based broadband RCS reduced super surface according to claim 2, wherein the dielectric plate thickness h of the first AMC unit, the second AMC unit is 2.4mm, the relative dielectric constant er = 4.4; the thickness t=0.035 mm of the upper metal structure of the first AMC unit and the second AMC unit.
4. A slot-loading based broadband RCS reduced super surface according to claim 3, wherein the length La = 7mm of the sides, the width Ws = 1.5mm of the sides, and the length Ls = 1mm of the slots parallel to the sides in the first square frame patch; the length li=3 mm of the sides in the first square patch; the length of the side in the second square frame patch is a=5.6mm; the length lc=2.27 mm of the side in the second square patch; the spacing Wa=0.4 mm between the edges of the second square frame patch and the second square patch, and at this time, the resonance frequency point of the first AMC unit is at 12GHz; the second AMC unit is a double-frequency annular artificial magnetic conductor unit, and resonance points are 8.5GHz and 17GHz respectively.
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