Tapered Resistive Sheets and FSS Absorber Loading for the Wideband RCS Reduction of the Elliptic Surface at TM Polarization
A wideband radar cross Section (RCS) reduction of the elliptic surface at TM polarization is reported in this communication. The main scattering sources and the corresponding scattering mechanisms of the elliptic surface are accurately identified based on the inverse synthetic aperture radar (ISAR)...
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Veröffentlicht in: | IEEE transactions on antennas and propagation 2023-07, Vol.71 (7), p.6191-6195 |
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creator | Huang, Ze Luo, Zhinan Zhao, Yong Li, Haoran Si, Kaixuan Han, Yi Miao, Ling Jiang, Jianjun |
description | A wideband radar cross Section (RCS) reduction of the elliptic surface at TM polarization is reported in this communication. The main scattering sources and the corresponding scattering mechanisms of the elliptic surface are accurately identified based on the inverse synthetic aperture radar (ISAR) imaging technique and the high-frequency approximation theory. The frequency selective surface (FSS) absorber is employed to suppress the specular reflection, and the tapered resistive sheets (TRSs) are used to handle the scattering from the trailing edges. Samples have been fabricated and measured in the anechoic room, both the simulation and measurement results illustrate that 10 dB RCS reduction (RCSR) is achieved within 1.35–4.9 GHz at TM polarization. |
doi_str_mv | 10.1109/TAP.2023.3265462 |
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The main scattering sources and the corresponding scattering mechanisms of the elliptic surface are accurately identified based on the inverse synthetic aperture radar (ISAR) imaging technique and the high-frequency approximation theory. The frequency selective surface (FSS) absorber is employed to suppress the specular reflection, and the tapered resistive sheets (TRSs) are used to handle the scattering from the trailing edges. Samples have been fabricated and measured in the anechoic room, both the simulation and measurement results illustrate that 10 dB RCS reduction (RCSR) is achieved within 1.35–4.9 GHz at TM polarization.</description><identifier>ISSN: 0018-926X</identifier><identifier>EISSN: 1558-2221</identifier><identifier>DOI: 10.1109/TAP.2023.3265462</identifier><language>eng</language><publisher>New York: The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</publisher><subject>Absorbers ; Broadband ; Frequency selective surfaces ; Imaging techniques ; Inverse synthetic aperture radar ; Polarization ; Radar cross sections ; Radar imaging ; Reduction ; Resistive sheets ; Scattering ; Specular reflection ; Trailing edges</subject><ispartof>IEEE transactions on antennas and propagation, 2023-07, Vol.71 (7), p.6191-6195</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. 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The main scattering sources and the corresponding scattering mechanisms of the elliptic surface are accurately identified based on the inverse synthetic aperture radar (ISAR) imaging technique and the high-frequency approximation theory. The frequency selective surface (FSS) absorber is employed to suppress the specular reflection, and the tapered resistive sheets (TRSs) are used to handle the scattering from the trailing edges. Samples have been fabricated and measured in the anechoic room, both the simulation and measurement results illustrate that 10 dB RCS reduction (RCSR) is achieved within 1.35–4.9 GHz at TM polarization.</description><subject>Absorbers</subject><subject>Broadband</subject><subject>Frequency selective surfaces</subject><subject>Imaging techniques</subject><subject>Inverse synthetic aperture radar</subject><subject>Polarization</subject><subject>Radar cross sections</subject><subject>Radar imaging</subject><subject>Reduction</subject><subject>Resistive sheets</subject><subject>Scattering</subject><subject>Specular reflection</subject><subject>Trailing edges</subject><issn>0018-926X</issn><issn>1558-2221</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNotkN1LwzAQwIMoOKfvPgZ87sxHP9LHMTYVJo61om8lTa4uoy41aQX1nzfV5eHCcb-7434IXVMyo5Tkt-V8M2OE8RlnaRKn7ARNaJKIiDFGT9GEECqinKWv5-jC-31IYxHHE_RTyg4caLwFb3xvPgEXO4DeY3nQeFUUeF5762pweG2lNoc33FiH-x3gF6OhHqntogjtelC9sQdsm7_qsm1N1xuFi8E1UgGWPS4f8ca20plvOaKX6KyRrYer4z9Fz6tlubiP1k93D4v5OlIso32ISmkClKg656lkmYYEag1cswZoOJczAiI8aFiTphREmok44ToWeZ4lwKfo5n9u5-zHAL6v9nZwh7CyYoLHPOhjWaDIP6Wc9d5BU3XOvEv3VVFSjYqroLgaFVdHxfwXkoZukQ</recordid><startdate>20230701</startdate><enddate>20230701</enddate><creator>Huang, Ze</creator><creator>Luo, Zhinan</creator><creator>Zhao, Yong</creator><creator>Li, Haoran</creator><creator>Si, Kaixuan</creator><creator>Han, Yi</creator><creator>Miao, Ling</creator><creator>Jiang, Jianjun</creator><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-9178-8988</orcidid><orcidid>https://orcid.org/0000-0001-5299-2433</orcidid></search><sort><creationdate>20230701</creationdate><title>Tapered Resistive Sheets and FSS Absorber Loading for the Wideband RCS Reduction of the Elliptic Surface at TM Polarization</title><author>Huang, Ze ; Luo, Zhinan ; Zhao, Yong ; Li, Haoran ; Si, Kaixuan ; Han, Yi ; Miao, Ling ; Jiang, Jianjun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c271t-c2ccd0e10cb936a27de5ebde3d2fe1326320e8888ef2f661e8678453d489975e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Absorbers</topic><topic>Broadband</topic><topic>Frequency selective surfaces</topic><topic>Imaging techniques</topic><topic>Inverse synthetic aperture radar</topic><topic>Polarization</topic><topic>Radar cross sections</topic><topic>Radar imaging</topic><topic>Reduction</topic><topic>Resistive sheets</topic><topic>Scattering</topic><topic>Specular reflection</topic><topic>Trailing edges</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Huang, Ze</creatorcontrib><creatorcontrib>Luo, Zhinan</creatorcontrib><creatorcontrib>Zhao, Yong</creatorcontrib><creatorcontrib>Li, Haoran</creatorcontrib><creatorcontrib>Si, Kaixuan</creatorcontrib><creatorcontrib>Han, Yi</creatorcontrib><creatorcontrib>Miao, Ling</creatorcontrib><creatorcontrib>Jiang, Jianjun</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>IEEE transactions on antennas and propagation</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Huang, Ze</au><au>Luo, Zhinan</au><au>Zhao, Yong</au><au>Li, Haoran</au><au>Si, Kaixuan</au><au>Han, Yi</au><au>Miao, Ling</au><au>Jiang, Jianjun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Tapered Resistive Sheets and FSS Absorber Loading for the Wideband RCS Reduction of the Elliptic Surface at TM Polarization</atitle><jtitle>IEEE transactions on antennas and propagation</jtitle><date>2023-07-01</date><risdate>2023</risdate><volume>71</volume><issue>7</issue><spage>6191</spage><epage>6195</epage><pages>6191-6195</pages><issn>0018-926X</issn><eissn>1558-2221</eissn><abstract>A wideband radar cross Section (RCS) reduction of the elliptic surface at TM polarization is reported in this communication. The main scattering sources and the corresponding scattering mechanisms of the elliptic surface are accurately identified based on the inverse synthetic aperture radar (ISAR) imaging technique and the high-frequency approximation theory. The frequency selective surface (FSS) absorber is employed to suppress the specular reflection, and the tapered resistive sheets (TRSs) are used to handle the scattering from the trailing edges. Samples have been fabricated and measured in the anechoic room, both the simulation and measurement results illustrate that 10 dB RCS reduction (RCSR) is achieved within 1.35–4.9 GHz at TM polarization.</abstract><cop>New York</cop><pub>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</pub><doi>10.1109/TAP.2023.3265462</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0001-9178-8988</orcidid><orcidid>https://orcid.org/0000-0001-5299-2433</orcidid></addata></record> |
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subjects | Absorbers Broadband Frequency selective surfaces Imaging techniques Inverse synthetic aperture radar Polarization Radar cross sections Radar imaging Reduction Resistive sheets Scattering Specular reflection Trailing edges |
title | Tapered Resistive Sheets and FSS Absorber Loading for the Wideband RCS Reduction of the Elliptic Surface at TM Polarization |
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