CN115000719A - Polarization conversion super surface - Google Patents
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Abstract
本申请涉及电磁隐身技术领域,特别涉及一种极化转换超表面。该极化转换超表面,包括:第一晶格和第二晶格;所述第一晶格由N×N个极化转换单元组成,所述极化转换单元包括沿竖直方向依次叠放的图案层、介质层和连续的底板层;其中,N≥2,所述图案层所在的一侧为电磁波入射的一侧,所述图案层中的图案为沿45°斜对角线对称的带有缝隙的图案,所述介质层用于协助所述图案层和所述底板层之间发生电磁耦合;所述第二晶格由所述第一晶格镜像而成;所述极化转换超表面由所述第一晶格和所述第二晶格按照预设的排布规律拼接而成。本申请提供的超表面可以将目标反射的电磁波均匀打散,显著缩减各向的RCS值。
The present application relates to the technical field of electromagnetic stealth, and in particular, to a polarization conversion metasurface. The polarization conversion metasurface includes: a first lattice and a second lattice; the first lattice is composed of N×N polarization conversion units, and the polarization conversion units are stacked in sequence along a vertical direction The pattern layer, the medium layer and the continuous bottom layer; wherein, N≥2, the side where the pattern layer is located is the side where the electromagnetic wave is incident, and the pattern in the pattern layer is symmetrical along a 45° diagonal line. a pattern with slits, the dielectric layer is used to assist electromagnetic coupling between the pattern layer and the base layer; the second lattice is formed by mirroring the first lattice; the polarization conversion The metasurface is formed by splicing the first lattice and the second lattice according to a preset arrangement rule. The metasurface provided by the present application can evenly disperse the electromagnetic waves reflected by the target, and significantly reduce the RCS value in all directions.
Description
技术领域technical field
本发明涉及电磁隐身技术领域,特别涉及一种极化转换超表面。The invention relates to the technical field of electromagnetic stealth, in particular to a polarization conversion metasurface.
背景技术Background technique
随着现代电子对抗与无线通信领域的发展,电磁隐身技术已经成为电磁学探索的热点之一。对于某些特殊应用场景的目标,其隐身性能的好坏直接影响到人们的安全性,因此如何降低目标被对方雷达等高科技设备侦测到的概率是研究者必须考虑到的问题。With the development of modern electronic countermeasures and wireless communication, electromagnetic stealth technology has become one of the hot spots of electromagnetic exploration. For targets in some special application scenarios, the quality of their stealth performance directly affects people's safety. Therefore, how to reduce the probability of the target being detected by the opponent's radar and other high-tech equipment is a problem that researchers must consider.
现有技术中,一般通过在目标表面设置极化转换超表面来缩减目标的RCS值,以降低目标被探测到的风险。然而,现有的极化转换超表面在缩减目标特定角域范围的RCS值时,会增加其他角域被侦测到的危险。In the prior art, the RCS value of the target is generally reduced by setting a polarization conversion metasurface on the target surface, so as to reduce the risk of the target being detected. However, when the existing polarization conversion metasurface reduces the RCS value in a specific angular domain of the target, it increases the risk of detection in other angular domains.
因此,目前亟待需要一种能够将目标反射的电磁波均匀打散的极化转换超表面,以缩减目标的各向RCS值。Therefore, there is an urgent need for a polarization conversion metasurface that can uniformly disperse the electromagnetic waves reflected by the target, so as to reduce the RCS value of the target in all directions.
发明内容SUMMARY OF THE INVENTION
本申请提供了一种极化转换超表面,能够在较宽的带宽范围内缩减目标的各向RCS值。The present application provides a polarization conversion metasurface capable of reducing the isotropic RCS value of a target in a wide bandwidth range.
本申请实施例提供了一种极化转换超表面,包括:第一晶格和第二晶格;Embodiments of the present application provide a polarization conversion metasurface, including: a first crystal lattice and a second crystal lattice;
所述第一晶格由N×N个极化转换单元组成,所述极化转换单元包括沿竖直方向依次叠放的图案层、介质层和连续的底板层;其中,N≥2,所述图案层所在的一侧为电磁波入射的一侧,所述图案层中的图案为沿45°斜对角线对称的带有缝隙的图案,所述介质层用于协助所述图案层和所述底板层之间发生电磁耦合;The first lattice is composed of N×N polarization conversion units, and the polarization conversion units include a pattern layer, a dielectric layer and a continuous bottom layer stacked in sequence along the vertical direction; wherein, N≥2, so the The side where the pattern layer is located is the side where the electromagnetic wave is incident, the pattern in the pattern layer is a pattern with slits symmetrical along a 45° oblique diagonal, and the dielectric layer is used to assist the pattern layer and all Electromagnetic coupling occurs between the bottom layers;
所述第二晶格由所述第一晶格镜像而成;the second lattice is formed by mirroring the first lattice;
所述极化转换超表面由所述第一晶格和所述第二晶格按照预设的排布规律拼接而成。The polarization conversion metasurface is formed by splicing the first crystal lattice and the second crystal lattice according to a preset arrangement rule.
在一种可能的设计中,所述极化转换单元的单元周期P=5mm;In a possible design, the unit period of the polarization conversion unit is P=5mm;
所述第一晶格由3×3个所述极化转换单元组成。The first lattice consists of 3×3 of the polarization conversion units.
在一种可能的设计中,所述图案层和所述底板层的材质为具有导电性的金属。In a possible design, the material of the pattern layer and the base layer is a metal with electrical conductivity.
在一种可能的设计中,所述金属为铜,所述铜的电导率为5.8×107S/m、厚度为0.035mm。In one possible design, the metal is copper, and the copper has a conductivity of 5.8×10 7 S/m and a thickness of 0.035 mm.
在一种可能的设计中,所述介质层的厚度为3mm、材质为F4B-220、介电常数为2.2C2/(N·M2)、介电损耗正切值为0.0015。In a possible design, the thickness of the dielectric layer is 3 mm, the material is F4B-220, the dielectric constant is 2.2C 2 /(N·M 2 ), and the dielectric loss tangent value is 0.0015.
在一种可能的设计中,所述图案层中的图案由一个斜45°条形结构和双环形结构组成,所述双环形结构由两个呈同心椭圆的开缝椭圆环组成,每个所述开缝椭圆环分别与所述条形结构相交并沿所述条形结构对称。In a possible design, the pattern in the pattern layer is composed of an oblique 45° strip structure and a double-ring structure, wherein the double-ring structure is composed of two concentric elliptical slit elliptical rings, each of which is The slotted elliptical rings respectively intersect with the strip-shaped structures and are symmetrical along the strip-shaped structures.
在一种可能的设计中,所述条形结构的长度L=6mm、宽度W=0.25mm。In a possible design, the length L=6mm and the width W=0.25mm of the strip structure.
在一种可能的设计中,所述开缝椭圆环由一个长轴内半径R1=2.4mm、线宽W1=0.2mm、轴比AR1=0.9、张角α=90°的第一开缝椭圆环和一个长轴内半径R2=0.3mm、线宽W2=0.3mm、轴比AR2=0.9、张角β=108°的第二开缝椭圆环组成。In a possible design, the slotted elliptical ring consists of a first axis with inner radius R 1 =2.4mm, line width W 1 =0.2mm, axial ratio AR 1 =0.9, and opening angle α=90° The slotted elliptical ring is composed of a second slotted elliptical ring with a major axis inner radius R 2 =0.3mm, a line width W 2 =0.3mm, an axial ratio AR 2 =0.9, and an opening angle β=108°.
在一种可能的设计中,所述预设的排布规律为将所述第一晶格和所述第二晶格均匀等间隔排布。In a possible design, the preset arrangement rule is to evenly arrange the first crystal lattice and the second crystal lattice at equal intervals.
在一种可能的设计中,所述预设的排布规律为以远场散射幅度的最大值为目标函数,通过遗传算法确定出的所述第一晶格和所述第二晶格的排布方式。In a possible design, the preset arrangement rule is that the arrangement of the first lattice and the second lattice determined by a genetic algorithm takes the maximum value of the far-field scattering amplitude as an objective function. cloth method.
本申请实施例提供了一种极化转换超表面,包括第一晶格和第二晶格,该第一晶格由N×N个极化转换单元组成,第二晶格由第一晶格镜像而成,如此可以形成周期结构,抑制极化转换单元之间的互耦;该极化转换单元包括沿竖直方向依次叠放的图案层、介质层和连续的底板层;一方面,由于图案层中的图案为沿45°斜对角线对称的带有缝隙的图案,因此,可以使电磁波沿45°斜对角线方向发生谐振,从而改变电磁波的极化方向并扩宽带宽;另一方面,由于第一晶格和第二晶格按照预设的排布规律拼接,因此可以将目标反射的电磁波均匀打散,显著缩减各向的RCS值。Embodiments of the present application provide a polarization conversion metasurface, including a first lattice and a second lattice, the first lattice is composed of N×N polarization conversion units, and the second lattice is composed of a first lattice In this way, a periodic structure can be formed and the mutual coupling between the polarization conversion units can be suppressed; the polarization conversion unit includes a pattern layer, a dielectric layer and a continuous bottom layer stacked in sequence along the vertical direction; on the one hand, due to the The pattern in the pattern layer is a symmetric pattern with a slit along a 45° diagonal line, so the electromagnetic wave can be resonated along the 45° diagonal direction, thereby changing the polarization direction of the electromagnetic wave and widening the bandwidth; On the one hand, since the first lattice and the second lattice are spliced according to a preset arrangement rule, the electromagnetic waves reflected by the target can be uniformly dispersed, and the RCS value in each direction can be significantly reduced.
附图说明Description of drawings
为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to illustrate the embodiments of the present invention or the technical solutions in the prior art more clearly, the following briefly introduces the accompanying drawings that need to be used in the description of the embodiments or the prior art. Obviously, the drawings in the following description are For some embodiments of the present invention, for those of ordinary skill in the art, other drawings can also be obtained according to these drawings without creative efforts.
图1是本发明一实施例提供的一种极化转换单元的侧视剖面图;1 is a side cross-sectional view of a polarization conversion unit according to an embodiment of the present invention;
图2是本发明一实施例提供的层案层示意图;2 is a schematic diagram of a layer pattern provided by an embodiment of the present invention;
图3是本发明一实施例提供的第一晶格宽带极化转换率曲线图;3 is a first lattice broadband polarization conversion rate curve diagram provided by an embodiment of the present invention;
图4是本发明一实施例提供的按照遗传算法确定出的优化编码结构极化转换超表面;4 is an optimized coding structure polarization conversion metasurface determined according to a genetic algorithm provided by an embodiment of the present invention;
图5是本发明一实施例提供的优化编码结构与均匀编码结构的单站RCS缩减对比图;5 is a comparison diagram of a single-station RCS reduction of an optimized coding structure and a uniform coding structure provided by an embodiment of the present invention;
图6是本发明一实施例提供的优化编码结构在13GHz处的3D远场散射方向图。FIG. 6 is a 3D far-field scattering pattern at 13 GHz of an optimized coding structure provided by an embodiment of the present invention.
附图标记:Reference number:
1-图案层;1- pattern layer;
11-条形结构;11-stripe structure;
12-第一开缝椭圆环;12- The first slotted oval ring;
13-第二开缝椭圆环;13- The second slotted oval ring;
2-介质层;2-dielectric layer;
3-底板层。3- Bottom layer.
具体实施方式Detailed ways
以下结合附图及实施例,对本申请进行详细说明。应当理解,此处所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。The present application will be described in 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.
在本申请实施例的描述中,除非另有明确的规定和限定,术语“第一”、“第二”仅用于描述的目的,而不能理解为指示或暗示相对重要性;除非另有规定或说明,术语“多个”是指两个或两个以上;术语“连接”、“固定”等均应做广义理解,例如,“连接”可以是固定连接,也可以是可拆卸连接,或一体地连接,或电连接;可以是直接相连,也可以通过中间媒介间接相连。对于本领域的普通技术人员而言,可以根据具体情况理解上述术语在本申请中的具体含义。In the description of the embodiments of the present application, unless otherwise explicitly specified and limited, the terms "first" and "second" are only used for the purpose of description, and cannot be understood as indicating or implying relative importance; unless otherwise specified Or to illustrate, the term "plurality" refers to two or more; the terms "connection" and "fixed" should be understood in a broad sense, for example, "connection" can be a fixed connection or a detachable connection, or Connected integrally, or connected electrically; it can be directly connected or indirectly connected through an intermediate medium. For those of ordinary skill in the art, the specific meanings of the above terms in this application can be understood according to specific situations.
本说明书的描述中,需要理解的是,本申请实施例所描述的“上”、“下”等方位词是以附图所示的角度来进行描述的,不应理解为对本申请实施例的限定。此外,在上下文中,还需要理解的是,当提到一个元件连接在另一个元件“上”或者“下”时,其不仅能够直接连接在另一个元件“上”或者“下”,也可以通过中间元件间接连接在另一个元件“上”或者“下”。In the description of this specification, it should be understood that the directional words such as "upper" and "lower" described in the embodiments of the present application are described from the perspective shown in the accompanying drawings, and should not be construed as referring to the embodiments of the present application. limited. Also, in this context, it should also be understood that when an element is referred to as being "on" or "under" another element, it can not only be directly connected "on" or "under" the other element, but also Indirectly connected "on" or "under" another element through intervening elements.
发明人在工作中发现,目前大多数极化转换超表面均采用棋盘型结构使入射电磁波与反射(透射)电磁波的反射相位差为180°,该结构能够通过相位对消的方法缩减平面目标的RCS值,但是同时会增加其他角域被侦测到的危险性。The inventors found in their work that most of the polarization conversion metasurfaces currently use a checkerboard structure to make the reflection phase difference between the incident electromagnetic wave and the reflected (transmitted) electromagnetic wave 180°. RCS value, but at the same time increases the risk of other angular domains being detected.
针对这一问题,发明人提出可以在极化转换单元中电磁波入射的一侧设置特殊的图案以及特殊的极化转换单元排布方式,将目标反射的电磁波均匀打散,从而缩减各向的RCS值。In response to this problem, the inventor proposes that a special pattern and a special arrangement of the polarization conversion units can be set on the side where the electromagnetic waves are incident in the polarization conversion unit, so as to evenly disperse the electromagnetic waves reflected by the target, thereby reducing the RCS in all directions value.
本申请实施例提供了一种极化转换超表面,包括:第一晶格和第二晶格;Embodiments of the present application provide a polarization conversion metasurface, including: a first crystal lattice and a second crystal lattice;
第一晶格由N×N个极化转换单元组成,如图1所示,极化转换单元包括沿竖直方向依次叠放的图案层1、介质层2和连续的底板层3;其中,N≥2,图案层1所在的一侧为电磁波入射的一侧,图案层中的图案为沿45°斜对角线对称的带有缝隙的图案,介质层2用于协助图案层1和底板层3之间发生电磁耦合;The first lattice is composed of N×N polarization conversion units. As shown in FIG. 1 , the polarization conversion unit includes a
第二晶格由第一晶格镜像而成;The second lattice is formed by mirroring the first lattice;
极化转换超表面由第一晶格和第二晶格按照预设的排布规律拼接而成。The polarization conversion metasurface is formed by splicing the first lattice and the second lattice according to a preset arrangement rule.
在该实施例中,第一晶格由N×N个极化转换单元组成,第二晶格由第一晶格镜像而成,如此可以形成周期结构,抑制极化转换单元之间的互耦;进一步地,由于图案层中的图案为沿45°斜对角线对称的带有缝隙的图案,因此,可以使电磁波沿45°斜对角线方向发生谐振,从而改变电磁波的极化方向并扩宽带宽;此外,由于第一晶格和第二晶格按照预设的排布规律拼接,因此可以将目标反射的电磁波均匀打散,显著缩减各向的RCS值。In this embodiment, the first lattice is composed of N×N polarization conversion units, and the second lattice is formed by mirroring the first lattice, so that a periodic structure can be formed and mutual coupling between the polarization conversion units can be suppressed Further, since the pattern in the pattern layer is a pattern with slits symmetrical along the 45° diagonal diagonal, the electromagnetic wave can be resonated along the 45° diagonal direction, thereby changing the polarization direction of the electromagnetic wave and Widen the bandwidth; in addition, since the first lattice and the second lattice are spliced according to the preset arrangement rule, the electromagnetic waves reflected by the target can be uniformly dispersed, and the RCS value in each direction can be significantly reduced.
可以理解的是,极化转换单元的单元周期越小,改变电磁波的极化方向以及扩宽带宽的效果越好,但对加工精度要求较高。因此,在一些实施方式中,在综合考虑加工制造的成本后,可以取极化转换单元的单元周期P=5mm。但由于该单元周期较小,各极化转换单元之间容易发生互耦,因此,在一些实施方式中,可以用3×3个极化转换单元组成第一晶格,第一晶格镜像形成第二晶格,如此在保证极化转化效果的同时,可以有效抑制极化转换单元之间的互耦。It can be understood that the smaller the unit period of the polarization conversion unit, the better the effect of changing the polarization direction of the electromagnetic wave and broadening the bandwidth, but requires higher processing accuracy. Therefore, in some embodiments, after comprehensively considering the manufacturing cost, the unit period of the polarization conversion unit may be taken as P=5mm. However, due to the small period of the unit, mutual coupling is likely to occur between the polarization conversion units. Therefore, in some embodiments, 3×3 polarization conversion units can be used to form the first lattice, and the first lattice is formed by a mirror image. The second crystal lattice can effectively suppress the mutual coupling between the polarization conversion units while ensuring the polarization conversion effect.
需要说明的是,单元周期P=5mm以及3×3个极化转换单元组成第一晶格只是一种优选方式,用户也可以根据对各向RCS值的缩减期望值进行调整,本申请并不以此为限。It should be noted that the unit period P=5mm and 3×3 polarization conversion units to form the first lattice is only a preferred way, and the user can also adjust it according to the expected reduction of the RCS value in each direction. This is limited.
在一些实施方式中,图案层1和底板层3的材质为具有导电性的金属。例如金、银、铜等,导电金属可以使图案层1和底板层3之间发生电磁耦合,形成环形电流,使电磁波产生谐振,从而有效扩宽带宽并产生极化转换。In some embodiments, the material of the
在一些实施方式中,综合考虑生产成本后,导电金属优选为铜,并取铜的电导率为5.8×107S/m、厚度为0.035mm。当然,用户也可以选择其它具有导电性的金属,本申请不做具体限定。In some embodiments, after comprehensively considering the production cost, the conductive metal is preferably copper, and the conductivity of copper is 5.8×10 7 S/m and the thickness is 0.035 mm. Of course, the user can also select other conductive metals, which are not specifically limited in this application.
在一些实施方式中,为了促进图案层1和底板层3之间发生电磁耦合并形成环形电流,需要在图案层1和底板层3之间设置介质层,介质层2的材料优选为材质为F4B-220、介电常数为2.2C2/(N·M2)、介电损耗正切值为0.0015,介质层2的厚度优选为3mm,如此可以保证极化转换超表面的柔性,增加超表面的适用范围。In some embodiments, in order to promote electromagnetic coupling between the
如图2所示,在一些实施方式中,图案层1中的图案由一个斜45°条形结构11和双环形结构组成,该双环形结构由两个呈同心椭圆的开缝椭圆环组成,每个开缝椭圆环分别与该条形结构11相交并沿该条形结构11对称。即沿极化转换单元主对角线(v轴)方向与副对角线(u轴)方向进行对称结构设计。该图案的设置可以增加电磁波沿45°斜对角线方向的谐振,最大限度的扩宽带宽和增加极化转换。As shown in FIG. 2 , in some embodiments, the pattern in the
图案确定之后,还需要对图案的物理参数进行优化,以实现极化转换单元u轴方向与v轴方向的特定幅频响应特性。在一种优选的方式中,该条形结构11的长度L=6mm、宽度W=0.25mm。开缝椭圆环由一个长轴内半径R1=2.4mm、线宽W1=0.2mm、轴比AR1=0.9、张角α=90°的第一开缝椭圆环12和一个长轴内半径R2=0.3mm、线宽W2=0.3mm、轴比AR2=0.9、张角β=108°的第二开缝椭圆环13组成。为了验证由该极化转换单元组成的第一晶格和第二晶格的极化转换率(PCR),发明人通过印刷电路板制备技术加工了由第一晶格组成的超表面的极化转换率测试板,并通过“拱形架+宽带双喇叭天线”测试系统分别测试极化转换率测试板的远场同极化反射率与交叉极化反射率,并通过公式计算出了实测宽带PCR曲线,如图3所示,从图中可以看出,采用上述物理参数后,由第一晶格组成的超表面能够实现8.03~22.16GHz频段内90%以上的线-交叉极化转换效率,即第一晶格能够实现8.03~22.16GHz频段内90%以上的线-交叉极化转换效率。由于第二晶格由第一晶格镜像而成,因此,第二晶格具有与第一晶格同样的效果。当然,上述尺寸只是一种优选的方式,本申请并不以此为限。After the pattern is determined, the physical parameters of the pattern also need to be optimized to achieve specific amplitude-frequency response characteristics in the u-axis and v-axis directions of the polarization conversion unit. In a preferred manner, the length L=6mm and the width W=0.25mm of the
极化转换单元的图案形式和尺寸确定之后,可以根据项目需求,微调各谐振频点的响应频率与作用带宽,将极化转换单元组成3×3的第一晶格和由第一晶格镜像而成的第二晶格。最后,为了更好的将目标反射的电磁波均匀打散,需要选择合适的第一晶格和第二晶格的排布方式。After the pattern form and size of the polarization conversion unit are determined, the response frequency and action bandwidth of each resonance frequency point can be fine-tuned according to the project requirements, and the polarization conversion unit can be composed of a 3×3 first lattice and a mirror image of the first lattice. The second lattice formed. Finally, in order to better uniformly disperse the electromagnetic waves reflected by the target, it is necessary to select an appropriate arrangement of the first lattice and the second lattice.
根据信息熵的概念可知,当组成极化转换超表面的第一晶格和第二晶格的数量各取一半时,其单站RCS缩减值最大。因此,在一些实施方式中,可以使第一晶格和第二晶格均匀等间隔排布,例如按照第一晶格、第二晶格、第一晶格、第二晶格……的排布方式,记为均匀编码,采用该均匀编码方式可以缩减目标大部分方向的RCS值,但是仍有极个别方向的RCS值缩减效果稍差。According to the concept of information entropy, when the number of the first lattice and the second lattice constituting the polarization conversion metasurface is half, the single-site RCS reduction value is the largest. Therefore, in some embodiments, the first crystal lattice and the second crystal lattice may be uniformly arranged at equal intervals, for example, according to the arrangement of the first crystal lattice, the second crystal lattice, the first crystal lattice, the second crystal lattice . . . The distribution method is denoted as uniform encoding. The uniform encoding method can reduce the RCS value in most directions of the target, but there are still very few directions in which the RCS value reduction effect is slightly worse.
如图4所示,在另一些实施方式中,可以以远场散射幅度的最大值为目标函数,通过遗传算法确定出第一晶格和第二晶格的排布方式,记为优化编码。具体地,将远场散射图幅度最大值作为目标函数,通过Matlab软件编写遗传算法程序,输出最优化第一晶格和第二晶格的布局矩阵,最终确定极化转换超表面的具体结构。采用该优化编码方式确定出的极化转换超表面,能够有效缩减目标各向的RCS值。As shown in FIG. 4 , in other embodiments, the maximum value of the far-field scattering amplitude may be used as the objective function, and the arrangement of the first lattice and the second lattice may be determined by a genetic algorithm, which is recorded as optimal coding. Specifically, taking the maximum amplitude of the far-field scattering map as the objective function, a genetic algorithm program was written by Matlab software to output the optimal layout matrix of the first lattice and the second lattice, and finally the specific structure of the polarization conversion metasurface was determined. The polarization conversion metasurface determined by this optimized coding method can effectively reduce the RCS value of the target in all directions.
为了验证图4所示的优化编码极化转换超表面的单站RCS减缩效果,发明人以尺寸为180mm×180mm×3mm的均匀编码极化转换超表面成品板作为实验组、以尺寸为180mm×180mm×3mm的优化编码极化转换超表面成品板作为实验组,分别通过自由空间法测试两种极化转换超表面成品板的单站RCS曲线,测试结果如图5所示,从图中可以看出,采用遗传算法确定出的优化编码确定出的超表面能够在9.82~23.15GHz频段内实现-10dB的单站RCS减缩,其缩减性能远远优于均匀编码结构。In order to verify the single-station RCS reduction effect of the optimized coding polarization conversion metasurface shown in Fig. 4, the inventors used a uniform coding polarization conversion metasurface finished board with a size of 180mm×180mm×3mm as the experimental group, and the size of 180mm× The 180mm×3mm optimized coding polarization conversion metasurface finished board was used as the experimental group, and the single-station RCS curves of the two polarization conversion metasurface finished boards were tested by the free space method. The test results are shown in Figure 5. It can be seen that the metasurface determined by the optimal coding determined by the genetic algorithm can achieve a single-station RCS reduction of -10dB in the frequency band of 9.82-23.15GHz, and its reduction performance is far better than that of the uniform coding structure.
另外,为了分析上述优化编码结构的单站RCS减缩机理,发明人选取13GHz频点的远场散射方向图,如图6所示,从图中可以看出入射波通过本发明的电磁作用后,将反射电磁波均匀打散成类似漫反射的形式,各向的RCS值均保持在-5.81~-15.8之间,大大缩减了威胁角域内被对方雷达探测到的概率。In addition, in order to analyze the single-station RCS reduction mechanism of the above-mentioned optimized coding structure, the inventor selected the far-field scattering pattern of the 13 GHz frequency point, as shown in FIG. The reflected electromagnetic waves are evenly dispersed into a form similar to diffuse reflection, and the RCS values in all directions are maintained between -5.81 and -15.8, which greatly reduces the probability of being detected by the opponent's radar in the threat angle domain.
还需要说明的是,为了保证测试结果的准确性,发明人在进行均匀编码超表面和优化编码超表面的RCS测量时,首先测量空室RCS,随后在测试台上放置相同尺寸的金属定标板,得到定标板的参考宽带RCS曲线,最后在测试台上放置待测试的成品板,得到待测试的成品板的实际单站RCS曲线,与定标板所得的实际数据相减,即可得到待测试成品板的宽带单站RCS缩减曲线,如此可以去除系统误差,保证测试结果的准确性。It should also be noted that, in order to ensure the accuracy of the test results, the inventors first measured the RCS of the empty chamber when performing the RCS measurement of the uniformly encoded metasurface and the optimized encoded metasurface, and then placed the same size metal calibration on the test bench. board, obtain the reference broadband RCS curve of the calibration board, and finally place the finished board to be tested on the test bench to obtain the actual single-station RCS curve of the finished board to be tested, and subtract the actual data obtained from the calibration board. The broadband single-station RCS reduction curve of the finished board to be tested is obtained, which can remove systematic errors and ensure the accuracy of the test results.
需要说明的是,在本文中,诸如第一和第二之类的关系术语仅仅用来将一个实体或者操作与另一个实体或操作区分开来,而不一定要求或者暗示这些实体或操作之间存在任何这种实际的关系或者顺序。而且,术语“包括”、“包含”或者其任何其他变体意在涵盖非排他性的包含,从而使得包括一系列要素的过程、方法、物品或者设备不仅包括那些要素,而且还包括没有明确列出的其他要素,或者是还包括为这种过程、方法、物品或者设备所固有的要素。在没有更多限制的情况下,由语句“包括一个…”限定的要素,并不排除在包括所述要素的过程、方法、物品或者设备中还存在另外的相同因素。It should be noted that, in this document, relational terms such as first and second are only used to distinguish one entity or operation from another entity or operation, and do not necessarily require or imply a relationship between these entities or operations. There is no such actual relationship or sequence. Moreover, the terms "comprising", "comprising" or any other variation thereof are intended to encompass a non-exclusive inclusion such that a process, method, article or device that includes a list of elements includes not only those elements, but also includes not explicitly listed or other elements inherent to such a process, method, article or apparatus. Without further limitation, an element qualified by the phrase "comprising a..." does not preclude the presence of additional identical elements in the process, method, article, or device that includes the element.
最后应说明的是:以上实施例仅用以说明本发明的技术方案,而非对其限制;尽管参照前述实施例对本发明进行了详细的说明,本领域的普通技术人员应当理解:其依然可以对前述各实施例所记载的技术方案进行修改,或者对其中部分技术特征进行等同替换;而这些修改或者替换,并不使相应技术方案的本质脱离本发明各实施例技术方案的精神和范围。Finally, it should be noted that the above embodiments are only used to illustrate the technical solutions of the present invention, but not to limit them; although the present invention has been described in detail with reference to the foregoing embodiments, those of ordinary skill in the art should understand that it can still be The technical solutions described in the foregoing embodiments are modified, or some technical features thereof are equivalently replaced; and these modifications or replacements do not make the essence of the corresponding technical solutions deviate from the spirit and scope of the technical solutions of the embodiments of the present invention.
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Citations (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6720936B1 (en) * | 2002-05-09 | 2004-04-13 | Bbnt Solutions Llc | Adaptive antenna system |
US20070280459A1 (en) * | 2006-06-06 | 2007-12-06 | Microsoft Corporation | Single button operations for a device |
CN108470973A (en) * | 2018-03-09 | 2018-08-31 | 南京航空航天大学 | Broadband RCS based on gap load reduces super surface |
US20190334220A1 (en) * | 2018-04-25 | 2019-10-31 | Texas Instruments Incorporated | Circularly-polarized dielectric waveguide launch for millimeter-wave data communication |
CN110797662A (en) * | 2019-06-04 | 2020-02-14 | 曲阜师范大学 | Broadband reflection type electromagnetic wave polarization rotating super surface |
CN113964538A (en) * | 2021-10-20 | 2022-01-21 | 中南大学 | Flexible RCS reduction device based on inhale integrative super surface of function that looses |
CN114267956A (en) * | 2021-12-21 | 2022-04-01 | 中国科学院光电技术研究所 | Subwavelength structure transflective metasurface device, beam scanning antenna and scanning method |
CN114336076A (en) * | 2022-01-13 | 2022-04-12 | 北京工业大学 | An Ultrathin Broadband RCS Reduced Coded Electromagnetic Metasurface |
-
2022
- 2022-05-12 CN CN202210515576.6A patent/CN115000719B/en active Active
Patent Citations (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6720936B1 (en) * | 2002-05-09 | 2004-04-13 | Bbnt Solutions Llc | Adaptive antenna system |
US20070280459A1 (en) * | 2006-06-06 | 2007-12-06 | Microsoft Corporation | Single button operations for a device |
CN108470973A (en) * | 2018-03-09 | 2018-08-31 | 南京航空航天大学 | Broadband RCS based on gap load reduces super surface |
US20190334220A1 (en) * | 2018-04-25 | 2019-10-31 | Texas Instruments Incorporated | Circularly-polarized dielectric waveguide launch for millimeter-wave data communication |
CN110797662A (en) * | 2019-06-04 | 2020-02-14 | 曲阜师范大学 | Broadband reflection type electromagnetic wave polarization rotating super surface |
CN113964538A (en) * | 2021-10-20 | 2022-01-21 | 中南大学 | Flexible RCS reduction device based on inhale integrative super surface of function that looses |
CN114267956A (en) * | 2021-12-21 | 2022-04-01 | 中国科学院光电技术研究所 | Subwavelength structure transflective metasurface device, beam scanning antenna and scanning method |
CN114336076A (en) * | 2022-01-13 | 2022-04-12 | 北京工业大学 | An Ultrathin Broadband RCS Reduced Coded Electromagnetic Metasurface |
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