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新型宽阻带频率选择表面的多功能拓扑结构和设计优化,适用于 X 波段、Ku 波段和毫米波应用。

Novel versatile topologies and design optimization of wide-bandstop frequency selective surfaces for X-band, Ku-band and millimeter-wave applications.

机构信息

Department of Engineering, Reykjavik University, Reykjavik, Iceland.

Faculty of Electronics, Telecommunications and Informatics, Gdansk University of Technology, Gdansk, Poland.

出版信息

Sci Rep. 2023 Feb 2;13(1):1952. doi: 10.1038/s41598-023-28922-4.

DOI:10.1038/s41598-023-28922-4
PMID:36732367
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9894983/
Abstract

Novel designs of frequency selective surface (FSS) are presented for wideband applications in X, Ku and mmWave (millimeter Wave) bands. Two identical metallic layers of FSS are imprinted on both sides of the RO4003 substrate. The geometry parameters are optimized to maximize the bandstop at the specified in-band maximum transmission level of -10 dB; satisfaction of the latter condition is enforced through appropriate formulation and handling of the design constraints. The proposed structure is versatile and can be readily re-designed for various operating bands. For the sake of illustration, two instances of the FSS were developed. Design 1 exhibits broad bandstop of 9.8 GHz at the X- and Ku-bands, whereas the bandstop of Design 2 is 33.5 GHz at the mmWave band. The two FSS unit cell designs share the same base topology, but specific dimensions are adjusted to operate within the lower and the higher bands, respectively. The unit cell is symmetrical, therefore, ensures an excellent resonance stability performance with respect to different polarizations (TE and TM) and incidence angles. For proof of concept only FSS Design 1 is fabricated and measured in an anechoic chamber. The simulated and measured results exhibit good agreement. Extensive benchmarking against state-of-the-art FSS designs from the literature corroborates the advantages of the proposed topology in terms of design novelty, topological versatility, compact size, and wide bandstop response as compared to the previously available designs.

摘要

提出了两种新颖的频率选择表面(FSS)设计,用于 X、Ku 和毫米波(mmWave)频段的宽带应用。FSS 的两个相同的金属层印在 RO4003 基底的两侧。通过优化几何参数,在指定的带内最大传输电平-10dB 处实现最大带阻;通过适当的公式和设计约束处理,强制满足后者的条件。所提出的结构具有通用性,可以很容易地重新设计用于各种工作频段。为了说明问题,设计了两种 FSS。设计 1 在 X 和 Ku 波段具有 9.8GHz 的宽带带阻,而设计 2 的带阻在毫米波波段为 33.5GHz。这两个 FSS 单元设计具有相同的基本拓扑结构,但具体尺寸分别进行了调整,以在较低和较高频段内工作。单元是对称的,因此可以确保在不同的极化(TE 和 TM)和入射角下具有出色的谐振稳定性性能。仅出于概念验证的目的,在消声室中制造和测量了 FSS 设计 1。模拟和测量结果吻合得很好。与文献中最新的 FSS 设计进行广泛的基准测试证实了与之前可用的设计相比,所提出的拓扑结构在设计新颖性、拓扑通用性、紧凑尺寸和宽带带阻响应方面具有优势。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/349e55d1820d/41598_2023_28922_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/cef18e26bead/41598_2023_28922_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/0ba69c1bb1ee/41598_2023_28922_Fig2_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/65fbc2ce23d9/41598_2023_28922_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/c7fc975ce0b2/41598_2023_28922_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/d7499cd5f57e/41598_2023_28922_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/0b7e86c860c6/41598_2023_28922_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/5c584912e036/41598_2023_28922_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/92ae6505dc85/41598_2023_28922_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/96c0526da3a2/41598_2023_28922_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/c845364d6544/41598_2023_28922_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/ca2724d56468/41598_2023_28922_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/349e55d1820d/41598_2023_28922_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/cef18e26bead/41598_2023_28922_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/0ba69c1bb1ee/41598_2023_28922_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/c5d261fa2f6f/41598_2023_28922_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/65fbc2ce23d9/41598_2023_28922_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/c7fc975ce0b2/41598_2023_28922_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/d7499cd5f57e/41598_2023_28922_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/0b7e86c860c6/41598_2023_28922_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/5c584912e036/41598_2023_28922_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/92ae6505dc85/41598_2023_28922_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/96c0526da3a2/41598_2023_28922_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/c845364d6544/41598_2023_28922_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/ca2724d56468/41598_2023_28922_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/87ff/9894983/349e55d1820d/41598_2023_28922_Fig13_HTML.jpg

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