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CN217903448U - Novel high temperature resistant frequency selection super surface structure - Google Patents

Novel high temperature resistant frequency selection super surface structure Download PDF

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CN217903448U
CN217903448U CN202222149919.XU CN202222149919U CN217903448U CN 217903448 U CN217903448 U CN 217903448U CN 202222149919 U CN202222149919 U CN 202222149919U CN 217903448 U CN217903448 U CN 217903448U
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metasurface
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dielectric
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封�波
袁琦
朱志标
蒋李鑫
蒋进明
李勇峰
屈绍波
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Air Force Engineering University of PLA
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Abstract

本实用新型公开了一种新型耐高温频率选择超表面结构,属于新型人工电磁材料技术领域,包括金属结构层和介质层,介质层包含介质上层和介质下层,介质上层和介质下层相互平行设置,金属结构层设置于介质上层和介质下层之间,且金属结构层分别与介质上层和介质下层相连接,金属结构层为耶路撒冷十字结构。本实用新型提供的新型耐高温频率选择超表面结构能够解决频率选择超表面结构在高温环境下的介电性能无法保持,从而无法完全满足现实工作环境需求的技术问题。

Figure 202222149919

The utility model discloses a novel high-temperature-resistant frequency-selective metasurface structure, which belongs to the technical field of new artificial electromagnetic materials, and includes a metal structure layer and a medium layer, the medium layer includes a medium upper layer and a medium lower layer, and the medium upper layer and the medium lower layer are arranged in parallel with each other. The metal structure layer is arranged between the upper layer of the medium and the lower layer of the medium, and the metal structure layer is respectively connected with the upper layer of the medium and the lower layer of the medium, and the metal structure layer is a Jerusalem cross structure. The novel high-temperature-resistant frequency-selective metasurface structure provided by the utility model can solve the technical problem that the dielectric properties of the frequency-selective metasurface structure cannot be maintained in a high-temperature environment, thereby failing to fully meet the requirements of the actual working environment.

Figure 202222149919

Description

一种新型耐高温频率选择超表面结构A Novel High Temperature Resistant Frequency Selective Metasurface Structure

技术领域technical field

本实用新型属于新型人工电磁材料技术领域,具体涉及一种新型耐高温频率选择超表面结构。The utility model belongs to the technical field of new artificial electromagnetic materials, and in particular relates to a novel high-temperature-resistant frequency-selective metasurface structure.

背景技术Background technique

电磁超表面是电磁超材料二维化、平面化的产物,由周期或准周期排列的亚波长尺寸单元结构组成,具有高效灵活的电磁调控能力,能广泛地运用于微波、红外、光学等领域。频率选择透波表面为电磁超表面的一种,针对透波频率的调控需求,频率选择透波表面具有透射频率选择功能,能够将需要的工作带内的电磁波透过表面结构,反射或者吸收工作带外电磁波,广泛运用在天线罩、空间滤波器、反射器等器件中。Electromagnetic metasurface is the product of two-dimensional and planarization of electromagnetic metamaterials. It is composed of periodic or quasi-periodic sub-wavelength unit structures. It has efficient and flexible electromagnetic control capabilities and can be widely used in microwave, infrared, optical and other fields. . The frequency-selective wave-transparent surface is a kind of electromagnetic metasurface. For the regulation of the wave-transmission frequency, the frequency-selective wave-transparent surface has a transmission frequency selection function, which can transmit the electromagnetic wave in the required working band through the surface structure, reflect or absorb the work. Out-of-band electromagnetic waves are widely used in radome, spatial filter, reflector and other devices.

目前电磁超表面设计技术发展迅速,常温下的电磁调控技术手段已经日渐完善。然而,目前常用的频率选择透波表面材料随着温度的升高,会发生如熔化、形变等变化,从而使超表面结构失去了原有的电磁性能,无法完全满足现实工作环境的需求。因此,有必要设计一种新型耐高温频率选择超表面结构。At present, the electromagnetic metasurface design technology is developing rapidly, and the electromagnetic control technology at room temperature has been gradually improved. However, the currently commonly used frequency-selective wave-transparent surface materials will undergo changes such as melting and deformation with the increase of temperature, so that the metasurface structure loses its original electromagnetic properties and cannot fully meet the needs of the actual working environment. Therefore, it is necessary to design a novel high-temperature-resistant frequency-selective metasurface structure.

实用新型内容Utility model content

本实用新型提供了一种新型耐高温频率选择超表面结构,旨在解决现有频率选择超表面结构在高温环境下的介电性能无法保持,从而无法完全满足现实工作环境需求的技术问题。The utility model provides a novel high-temperature-resistant frequency-selective metasurface structure, aiming at solving the technical problem that the dielectric properties of the existing frequency-selective metasurface structure cannot be maintained in a high-temperature environment, thereby failing to fully meet the requirements of the actual working environment.

为实现上述目的,本实用新型采用的技术方案是:For realizing above-mentioned object, the technical scheme that the utility model adopts is:

一种新型耐高温频率选择超表面结构,包括金属结构层和介质层,介质层包含介质上层和介质下层,介质上层和介质下层相互平行设置,金属结构层设置于介质上层和介质下层之间,且金属结构层分别与介质上层和介质下层相连接,金属结构层为耶路撒冷十字结构。A novel high-temperature-resistant frequency-selective metasurface structure, including a metal structure layer and a dielectric layer, the dielectric layer includes a dielectric upper layer and a dielectric lower layer, the upper dielectric layer and the lower dielectric layer are arranged parallel to each other, and the metal structure layer is arranged between the upper dielectric layer and the lower dielectric layer, And the metal structure layer is respectively connected with the medium upper layer and the medium lower layer, and the metal structure layer is a Jerusalem cross structure.

优选的,金属结构层的单元结构周期长度p=6mm,厚度d=0.4mm,耶路撒冷十字结构的长度a=5mm,宽度b=2.2mm,金属线宽w=0.3mm,金属结构层的厚度t=0.02mm。Preferably, the unit structure period length of the metal structure layer is p=6mm, the thickness d=0.4mm, the length a of the Jerusalem cross structure is a=5mm, the width b=2.2mm, the metal line width w=0.3mm, and the thickness of the metal structure layer is t = 0.02mm.

优选的,介质上层的厚度d1与介质下层d2的厚度相同。Preferably, the thickness d1 of the upper layer of the medium is the same as the thickness of the lower layer d2 of the medium.

进一步优选的,d1=d2=0.2mm。Further preferably, d1=d2=0.2mm.

优选的,金属结构层的材质为固态金属钨。Preferably, the material of the metal structure layer is solid metal tungsten.

优选的,介质上层和介质下层的材质均为氮化铝陶瓷。Preferably, the upper dielectric layer and the lower dielectric layer are made of aluminum nitride ceramics.

本实用新型与现有技术相比,其有益效果在于:Compared with the prior art, the utility model has the beneficial effects of:

(1)本实用新型提供的新型耐高温频率选择超表面结构通过金属结构层的特殊结构设计,并通过金属结构层的特殊尺寸,例如周期、厚度、金属长度、宽度等特殊尺寸设计,能够实现工作频率的移动以及工作强度的变化,对于频率和效率的可调性强。(1) The novel high-temperature-resistant frequency-selective metasurface structure provided by the utility model can realize The movement of working frequency and the change of working intensity are highly adjustable for frequency and efficiency.

(2)本实用新型的结构具有耐高温能力,在室温~900℃环境下,X波段反射性能与K波段透射性能稳定。(2) The structure of the utility model has high temperature resistance, and the X-band reflection performance and K-band transmission performance are stable in the environment of room temperature to 900°C.

(3)本实用新型的结构具有抗氧化能力,在900℃环境维持10分钟退热后电磁参数维持稳定。(3) The structure of the utility model has anti-oxidation ability, and the electromagnetic parameters remain stable after the temperature is reduced for 10 minutes at 900°C.

附图说明Description of drawings

图1为本实用新型实施例提供的耐高温频率选择超表面结构在分解状态下的结构示意图。Fig. 1 is a schematic structural diagram of a high-temperature-resistant frequency-selective metasurface structure in a decomposed state provided by an embodiment of the present invention.

图2为本实用新型实施例中的金属层的结构示意图。FIG. 2 is a schematic structural diagram of a metal layer in an embodiment of the present invention.

图3为本实用新型实施例提供的耐高温频率选择超表面结构的右视剖面图。Fig. 3 is a right side sectional view of the high temperature resistant frequency selective metasurface structure provided by the embodiment of the present invention.

图4为本实用新型实施例提供的耐高温频率选择超表面结构的20×20结构单元样品图。Fig. 4 is a sample diagram of a 20×20 structural unit of the high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the utility model.

图5为本实用新型实施例提供的耐高温频率选择超表面结构在不同温度下的S参数仿真曲线图。Fig. 5 is a simulation curve diagram of S parameters at different temperatures for the high temperature resistant frequency selective metasurface structure provided by the embodiment of the present invention.

图6为本实用新型实施例提供的耐高温频率选择超表面结构在不同温度下的透射率测试曲线图。Fig. 6 is a test curve of transmittance at different temperatures of the high temperature resistant frequency selective metasurface structure provided by the embodiment of the present invention.

图7为本实用新型实施例提供的耐高温频率选择超表面结构在900℃环境和y极化电磁波入射下于不同频率下的电流分布图;Fig. 7 is the current distribution diagram of the high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the present invention at different frequencies under the environment of 900°C and the incidence of y-polarized electromagnetic waves;

其中,图7(a)为9.45GHz处的电流沿y分量的分布图;图7(b)为15.10GHz处的电流沿y分量的分布图;Among them, Figure 7(a) is a distribution diagram of the current at 9.45GHz along the y component; Figure 7(b) is a distribution diagram of the current at 15.10GHz along the y component;

图中:1、介质上层;2、金属结构层;3、介质下层。In the figure: 1. The upper layer of the medium; 2. The metal structure layer; 3. The lower layer of the medium.

具体实施方式Detailed ways

为了更清楚地说明本实用新型实施例及其设计方案,下面将对本实施例所需的附图作简单地介绍。下面描述中的附图仅仅是本实用新型的部分实施例,对于本领域普通技术人员来说,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 embodiment of the utility model and its design scheme more clearly, the accompanying drawings required by the embodiment will be briefly introduced below. The drawings in the following description are only part of the embodiments of the present utility model, and those skilled in the art can also obtain other drawings according to these drawings without creative work.

实施例1Example 1

如图1至图4所示,本实用新型实施例提供的新型耐高温频率选择超表面结构,包括金属结构层2和介质层,介质层包含介质上层1和介质下层3,介质上层1和介质下层3相互平行设置,金属结构层2设置于介质上层1和介质下层3之间,且金属结构层2分别与介质上层1和介质下层3相连接,其特征在于,所述金属结构层2为耶路撒冷十字结构,本实用新型实施例通过将金属结构层设计为特殊的耶路撒冷十字结构,由于金属耶路撒冷十字结构的等效电路模型中具有电容、电感以及电阻,所以通过将耶路撒冷十字结构特殊的尺寸参数设计能够改变超表面结构的等效电容值、电感值从而实现频率选择谐振频率的控制。As shown in Figures 1 to 4, the novel high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the present invention includes a metal structure layer 2 and a dielectric layer, the dielectric layer includes a dielectric upper layer 1 and a dielectric lower layer 3, and a dielectric upper layer 1 and a dielectric layer The lower layers 3 are arranged parallel to each other, the metal structure layer 2 is arranged between the upper dielectric layer 1 and the lower dielectric layer 3, and the metal structure layer 2 is connected to the upper dielectric layer 1 and the lower dielectric layer 3 respectively, and the metal structure layer 2 is Jerusalem cross structure, the embodiment of the utility model designs the metal structure layer as a special Jerusalem cross structure. Since the equivalent circuit model of the metal Jerusalem cross structure has capacitance, inductance and resistance, the special size parameters of the Jerusalem cross structure The design can change the equivalent capacitance value and inductance value of the metasurface structure to realize the control of frequency selective resonance frequency.

本实用新型实施例提供的新型耐高温频率选择超表面结构的制备方法,包括以下步骤:The preparation method of the novel high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the utility model includes the following steps:

(1)通过生瓷片层压形成介质下层3;(1) Forming the dielectric lower layer 3 by laminating green ceramic sheets;

(2)在介质下层3的表面通过印刷丝网工艺印刷金属结构层2;(2) Printing the metal structure layer 2 on the surface of the medium lower layer 3 through a printing screen process;

(3)通过生瓷片在金属结构层2和介质下层3的表面层压覆盖得到介质上层1,最后烧结成型得到新型耐高温频率选择超表面结构。本实用新型实施例得到的新型耐高温频率选择超表面结构中的介质上层1和介质下层3之间无缝隙,为一体结构,金属结构层2设置于介质上层1和介质下层3之间的夹层中。(3) The upper dielectric layer 1 is obtained by laminating and covering the surface of the metal structure layer 2 and the lower dielectric layer 3 with green ceramic sheets, and finally sintered to obtain a new high-temperature-resistant frequency-selective metasurface structure. In the novel high-temperature-resistant frequency-selective metasurface structure obtained in the embodiment of the present utility model, there is no gap between the upper dielectric layer 1 and the lower dielectric layer 3, which is an integrated structure, and the metal structure layer 2 is arranged in the interlayer between the upper dielectric layer 1 and the lower dielectric layer 3 middle.

本实用新型实施例上述制备工艺为现有工艺,具体可参考公开号为CN109053196B的发明专利中共烧陶瓷的制备工艺。The above-mentioned preparation process of the embodiment of the utility model is an existing process, and for details, reference may be made to the preparation process of co-fired ceramics in the invention patent with publication number CN109053196B.

金属结构层2的单元结构周期长度p=6mm,厚度d=0.4mm,耶路撒冷十字结构的长度a=5mm,宽度b=2.2mm,金属线宽w=0.3mm,金属结构层2的厚度t=0.02mm。The unit structure period length of the metal structure layer 2 is p=6mm, the thickness d=0.4mm, the length a=5mm of the Jerusalem cross structure, the width b=2.2mm, the metal line width w=0.3mm, and the thickness t of the metal structure layer 2= 0.02mm.

介质上层1的厚度d1与介质下层3的厚度d2相同。d1=d2=0.2mm。The thickness d1 of the dielectric upper layer 1 is the same as the thickness d2 of the dielectric lower layer 3 . d1 = d2 = 0.2 mm.

金属结构层2的材质为固态金属钨。固态金属钨的熔点大于3000℃,导电率为1.88×107S/m,在900℃内,使得夹层结构能够具有抗氧化、保持良好的金属导电性能。The material of the metal structure layer 2 is solid metal tungsten. The melting point of solid metal tungsten is greater than 3000°C, and the conductivity is 1.88×10 7 S/m. Within 900°C, the sandwich structure can resist oxidation and maintain good metal conductivity.

介质上层1和介质下层3的材质均为氮化铝陶瓷。The materials of the upper dielectric layer 1 and the lower dielectric layer 3 are aluminum nitride ceramics.

本实用新型实施例对介质上层1和介质下层3在不同温度下的电磁性能进行了测试,具体通过高温波导腔(型号为RETRL0812HT1000)在不同温度下测得,通过将介质上层1和介质下层3分别切割成X与Ku波段需要的尺寸进行波导测试得出的,测试结果为:The embodiment of the utility model tests the electromagnetic properties of the upper dielectric layer 1 and the lower dielectric layer 3 at different temperatures. It is obtained by cutting into the dimensions required by the X and Ku bands for waveguide testing. The test results are:

介质上层1和介质下层3在室温环境下、8~18GHz范围内的相对介电常数为7.8±0.1,介电损耗角正切为0.006±0.002。The dielectric upper layer 1 and the dielectric lower layer 3 have a relative permittivity of 7.8±0.1 and a dielectric loss tangent of 0.006±0.002 at room temperature within the range of 8-18GHz.

介质上层1和介质下层3在300℃、8~18GHz范围内的相对介电常数为7.8±0.1,介电损耗角正切为0.012±0.002。The dielectric upper layer 1 and the dielectric lower layer 3 have a relative permittivity of 7.8±0.1 and a dielectric loss tangent of 0.012±0.002 in the range of 300°C and 8-18GHz.

介质上层1和介质下层3在600℃、8~18GHz范围内的相对介电常数为7.8±0.1,介电损耗角正切为0.014±0.003。The dielectric upper layer 1 and the dielectric lower layer 3 have a relative permittivity of 7.8±0.1 and a dielectric loss tangent of 0.014±0.003 in the range of 600° C. and 8-18 GHz.

介质上层1和介质下层3在900℃、8~18GHz范围内的相对介电常数为7.8±0.1,介电损耗角正切为0.027±0.003。The dielectric upper layer 1 and the dielectric lower layer 3 have a relative permittivity of 7.8±0.1 and a dielectric loss tangent of 0.027±0.003 in the range of 900°C and 8-18GHz.

通过上述电磁性能的测试结果说明介质的介电参数随温度变化保持相对稳定。The test results of the above electromagnetic properties show that the dielectric parameters of the medium remain relatively stable with temperature changes.

为了验证本实用新型实施例提供的新型耐高温频率选择超表面结构的效果,下面进行仿真模拟和实验验证。In order to verify the effect of the novel high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the utility model, simulation and experimental verification are carried out below.

图5为本实用新型实施例提供的耐高温频率选择超表面结构在不同温度下线极化波入射的S参数曲线。仿真过程在CST微波工作室中进行,其中S11表示反射曲线,S21表示透射曲线。从室温到900℃变化过程中,S参数曲线没有发生明显的变化,说明了本实用新型实施例提供的耐高温频率选择超表面结构在高温下频率选择的稳定性,即X波段反射与K波段透射。Fig. 5 is the S-parameter curves of the high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the present invention at different temperatures when linearly polarized waves are incident. The simulation process is carried out in the CST microwave studio, where S11 represents the reflection curve, and S21 represents the transmission curve. During the change process from room temperature to 900°C, the S parameter curve does not change significantly, which illustrates the stability of the frequency selection of the high temperature resistant frequency selection metasurface structure provided by the embodiment of the present invention at high temperature, that is, the X-band reflection and the K-band transmission.

图6为本实用新型实施例提供的耐高温频率选择超表面结构在不同温度下y极化波入射的透射率测试曲线。测试过程中,将结构样品放置在石英加热箱中,在室温、300℃、600℃和900℃温度测试点保温10分钟后分别进行透射率测试,在不同温度下的测试曲线结果相近,验证了仿真结果和设计理论,证实了本实用新型实施例提供的耐高温频率选择超表面结构具有抗氧化能力,在高温环境下电磁参数维持稳定。Fig. 6 is a test curve of transmittance of y-polarized wave incidence at different temperatures of the high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the present invention. During the test, the structural sample was placed in a quartz heating box, and the transmittance test was performed at room temperature, 300°C, 600°C and 900°C temperature test points for 10 minutes, and the test curve results at different temperatures were similar, which verified the The simulation results and the design theory prove that the high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the utility model has anti-oxidation ability, and the electromagnetic parameters remain stable in a high-temperature environment.

此外,如图7所示,本实用新型实施例提供的耐高温频率选择超表面结构在900℃环境和y极化电磁波入射下于不同频率处的电流分布结果如图7所示,通过图7可以看出,当频率为15.1GHz(工作频率)时,耐高温频率选择超表面结构的表面电流分布强,体现出了强谐振效应;而当频率为9.45GHz(非工作频率)时,耐高温频率选择超表面结构的表面电流分布弱,此时超表面无透波效果。同时当频率为15.1GHz时,电流主要分布在y轴,对应了y极化入射(x轴无电流),说明了耐高温频率选择超表面结构在透射时发挥了良好的作用。In addition, as shown in Figure 7, the current distribution results at different frequencies of the high-temperature-resistant frequency-selective metasurface structure provided by the embodiment of the utility model are shown in Figure 7 under the environment of 900 ° C and the incidence of y-polarized electromagnetic waves. It can be seen that when the frequency is 15.1GHz (operating frequency), the surface current distribution of the high-temperature-resistant frequency-selective metasurface structure is strong, reflecting a strong resonance effect; and when the frequency is 9.45GHz (non-operating frequency), the high-temperature-resistant The surface current distribution of the frequency selective metasurface structure is weak, and the metasurface has no wave-transmitting effect at this time. At the same time, when the frequency is 15.1 GHz, the current is mainly distributed on the y-axis, corresponding to the y-polarized incident (no current on the x-axis), indicating that the high-temperature-resistant frequency-selective metasurface structure plays a good role in transmission.

尽管已经示出和描述了本实用新型的实施例,本领域的普通技术人员可以理解:在不脱离本实用新型的原理和宗旨的情况下可以对这些实施例进行多种变化、修改、替换和变型,本实用新型的范围由权利要求及其等同物限定。Although the embodiments of the present invention have been shown and described, those skilled in the art can understand that various changes, modifications, substitutions and modifications, the scope of the present invention is defined by the claims and their equivalents.

Claims (6)

1.一种新型耐高温频率选择超表面结构,包括金属结构层(2)和介质层,介质层包含介质上层(1)和介质下层(3),介质上层(1)和介质下层(3)相互平行设置,金属结构层(2)设置于介质上层(1)和介质下层(3)之间,且金属结构层(2)分别与介质上层(1)和介质下层(3)相连接,其特征在于,所述金属结构层(2)为耶路撒冷十字结构。1. A new type of high temperature resistant frequency selective metasurface structure, including a metal structure layer (2) and a dielectric layer, the dielectric layer includes a dielectric upper layer (1) and a dielectric lower layer (3), a dielectric upper layer (1) and a dielectric lower layer (3) Arranged parallel to each other, the metal structure layer (2) is arranged between the upper dielectric layer (1) and the lower dielectric layer (3), and the metal structure layer (2) is connected to the upper dielectric layer (1) and the lower dielectric layer (3) respectively, the The feature is that the metal structure layer (2) is a Jerusalem cross structure. 2.如权利要求1所述的新型耐高温频率选择超表面结构,其特征在于,所述金属结构层(2)的单元结构周期长度p=6mm,厚度d=0.4mm,耶路撒冷十字结构的长度a=5mm,宽度b=2.2mm,金属线宽w=0.3mm,金属结构层(2)的厚度t=0.02mm。2. novel high-temperature resistant frequency selective metasurface structure as claimed in claim 1, is characterized in that, the unit structure periodic length p=6mm of described metal structure layer (2), thickness d=0.4mm, the length of Jerusalem cross structure a=5mm, width b=2.2mm, metal line width w=0.3mm, thickness t=0.02mm of the metal structure layer (2). 3.如权利要求1所述的新型耐高温频率选择超表面结构,其特征在于,所述介质上层(1)的厚度d1与介质下层(3)的厚度d2相同。3. The novel high temperature resistant frequency selective metasurface structure according to claim 1, characterized in that the thickness d1 of the upper dielectric layer (1) is the same as the thickness d2 of the lower dielectric layer (3). 4.如权利要求3所述的新型耐高温频率选择超表面结构,其特征在于,所述d1=d2=0.2mm。4. The novel high temperature resistant frequency selective metasurface structure according to claim 3, characterized in that d1=d2=0.2mm. 5.如权利要求1所述的新型耐高温频率选择超表面结构,其特征在于,所述金属结构层(2)的材质为固态金属钨。5. The novel high temperature resistant frequency selective metasurface structure according to claim 1, characterized in that the metal structure layer (2) is made of solid metal tungsten. 6.如权利要求1所述的新型耐高温频率选择超表面结构,其特征在于,所述介质上层(1)和介质下层(3)的材质均为氮化铝陶瓷。6. The novel high-temperature-resistant frequency-selective metasurface structure according to claim 1, characterized in that the materials of the upper dielectric layer (1) and the lower dielectric layer (3) are aluminum nitride ceramics.
CN202222149919.XU 2022-08-16 2022-08-16 Novel high temperature resistant frequency selection super surface structure Expired - Fee Related CN217903448U (en)

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PL447615A1 (en) * 2024-01-26 2025-07-28 Zachodniopomorski Uniwersytet Technologiczny W Szczecinie Terahertz metasurface

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
PL447615A1 (en) * 2024-01-26 2025-07-28 Zachodniopomorski Uniwersytet Technologiczny W Szczecinie Terahertz metasurface

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