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A high‐gain circularly polarized Fabry‐Perot antenna with chiral metamaterial‐based circular polarizer
A high‐gain circularly polarized Fabry‐Perot (FP) antenna with chiral metamaterial (CMM)‐based circular polarizer is presented in this paper. It consists of two cavities. One is a U‐shaped slot microstrip antenna with a partially reflecting surface (PRS), acting as an FP cavity. The other is compose...
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Published in: | Microwave and optical technology letters 2020-02, Vol.62 (2), p.906-911 |
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creator | Hu, Yan‐wen Wang, Yu Yan, Zhong‐ming Zhou, Hong‐cheng |
description | A high‐gain circularly polarized Fabry‐Perot (FP) antenna with chiral metamaterial (CMM)‐based circular polarizer is presented in this paper. It consists of two cavities. One is a U‐shaped slot microstrip antenna with a partially reflecting surface (PRS), acting as an FP cavity. The other is composed of PRS and CMM plate which act as a circular polarizer. According to the experimental results, within the impedance bandwidth of 0.63 GHz from 8.71 to 9.34 GHz, the axial ratio and reflection coefficient S11 of the antenna are less than 3 and −10 dB, respectively. At 9 GHz, the maximum gains of simulation and measurement are 18.5 and 18.3 dB, respectively. The measurement results are according well with the simulation results. Similar methods can be extended to other bands to design high‐gain circularly polarized antennas. |
doi_str_mv | 10.1002/mop.32102 |
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It consists of two cavities. One is a U‐shaped slot microstrip antenna with a partially reflecting surface (PRS), acting as an FP cavity. The other is composed of PRS and CMM plate which act as a circular polarizer. According to the experimental results, within the impedance bandwidth of 0.63 GHz from 8.71 to 9.34 GHz, the axial ratio and reflection coefficient S11 of the antenna are less than 3 and −10 dB, respectively. At 9 GHz, the maximum gains of simulation and measurement are 18.5 and 18.3 dB, respectively. The measurement results are according well with the simulation results. Similar methods can be extended to other bands to design high‐gain circularly polarized antennas.</description><identifier>ISSN: 0895-2477</identifier><identifier>EISSN: 1098-2760</identifier><identifier>DOI: 10.1002/mop.32102</identifier><language>eng</language><publisher>Hoboken, USA: John Wiley & Sons, Inc</publisher><subject>antenna ; chiral metamaterial ; Circular polarization ; Fabry‐Perot ; high‐gain ; Holes ; Metamaterials ; Microstrip antennas ; partially reflecting surface ; Polarizers ; Reflectance</subject><ispartof>Microwave and optical technology letters, 2020-02, Vol.62 (2), p.906-911</ispartof><rights>2019 Wiley Periodicals, Inc.</rights><rights>2020 Wiley Periodicals, Inc.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c2972-38403196ea1c4e99823c6291bbd018c2ef2051218b7ca5238ea7c415b578a9793</citedby><cites>FETCH-LOGICAL-c2972-38403196ea1c4e99823c6291bbd018c2ef2051218b7ca5238ea7c415b578a9793</cites><orcidid>0000-0003-1557-6064</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Hu, Yan‐wen</creatorcontrib><creatorcontrib>Wang, Yu</creatorcontrib><creatorcontrib>Yan, Zhong‐ming</creatorcontrib><creatorcontrib>Zhou, Hong‐cheng</creatorcontrib><title>A high‐gain circularly polarized Fabry‐Perot antenna with chiral metamaterial‐based circular polarizer</title><title>Microwave and optical technology letters</title><description>A high‐gain circularly polarized Fabry‐Perot (FP) antenna with chiral metamaterial (CMM)‐based circular polarizer is presented in this paper. It consists of two cavities. One is a U‐shaped slot microstrip antenna with a partially reflecting surface (PRS), acting as an FP cavity. The other is composed of PRS and CMM plate which act as a circular polarizer. According to the experimental results, within the impedance bandwidth of 0.63 GHz from 8.71 to 9.34 GHz, the axial ratio and reflection coefficient S11 of the antenna are less than 3 and −10 dB, respectively. At 9 GHz, the maximum gains of simulation and measurement are 18.5 and 18.3 dB, respectively. The measurement results are according well with the simulation results. Similar methods can be extended to other bands to design high‐gain circularly polarized antennas.</description><subject>antenna</subject><subject>chiral metamaterial</subject><subject>Circular polarization</subject><subject>Fabry‐Perot</subject><subject>high‐gain</subject><subject>Holes</subject><subject>Metamaterials</subject><subject>Microstrip antennas</subject><subject>partially reflecting surface</subject><subject>Polarizers</subject><subject>Reflectance</subject><issn>0895-2477</issn><issn>1098-2760</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNp10L1OwzAUBWALgUQpDLxBJCaGtNfXSW2PVUUBqYgOMFuO6zau8oeTqioTj8Az8iQYAmxMZ_nuudIh5JLCiALguKybEUMKeEQGFKSIkU_gmAxAyDTGhPNTcta2WwBgnOOAFNMod5v84-19o10VGefNrtC-OERNHdK92lU015k_BLG0vu4iXXW2qnS0d10emdx5XUSl7XSpO-udLgLMdBvOfrv-mvw5OVnrorUXPzkkz_Obp9ldvHi8vZ9NF7FByTFmIgFG5cRqahIrpUBmJihplq2ACoN2jZBSpCLjRqfIhNXcJDTNUi605JINyVXf2_j6ZWfbTm3rna_CS4WMIdAAIajrXhlft623a9V4V2p_UBTU15gqjKm-xwx23Nu9K-zhf6geHpf9xSdZWnlZ</recordid><startdate>202002</startdate><enddate>202002</enddate><creator>Hu, Yan‐wen</creator><creator>Wang, Yu</creator><creator>Yan, Zhong‐ming</creator><creator>Zhou, Hong‐cheng</creator><general>John Wiley & Sons, Inc</general><general>Wiley Subscription Services, Inc</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-1557-6064</orcidid></search><sort><creationdate>202002</creationdate><title>A high‐gain circularly polarized Fabry‐Perot antenna with chiral metamaterial‐based circular polarizer</title><author>Hu, Yan‐wen ; Wang, Yu ; Yan, Zhong‐ming ; Zhou, Hong‐cheng</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2972-38403196ea1c4e99823c6291bbd018c2ef2051218b7ca5238ea7c415b578a9793</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>antenna</topic><topic>chiral metamaterial</topic><topic>Circular polarization</topic><topic>Fabry‐Perot</topic><topic>high‐gain</topic><topic>Holes</topic><topic>Metamaterials</topic><topic>Microstrip antennas</topic><topic>partially reflecting surface</topic><topic>Polarizers</topic><topic>Reflectance</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hu, Yan‐wen</creatorcontrib><creatorcontrib>Wang, Yu</creatorcontrib><creatorcontrib>Yan, Zhong‐ming</creatorcontrib><creatorcontrib>Zhou, Hong‐cheng</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Microwave and optical technology letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hu, Yan‐wen</au><au>Wang, Yu</au><au>Yan, Zhong‐ming</au><au>Zhou, Hong‐cheng</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A high‐gain circularly polarized Fabry‐Perot antenna with chiral metamaterial‐based circular polarizer</atitle><jtitle>Microwave and optical technology letters</jtitle><date>2020-02</date><risdate>2020</risdate><volume>62</volume><issue>2</issue><spage>906</spage><epage>911</epage><pages>906-911</pages><issn>0895-2477</issn><eissn>1098-2760</eissn><abstract>A high‐gain circularly polarized Fabry‐Perot (FP) antenna with chiral metamaterial (CMM)‐based circular polarizer is presented in this paper. It consists of two cavities. One is a U‐shaped slot microstrip antenna with a partially reflecting surface (PRS), acting as an FP cavity. The other is composed of PRS and CMM plate which act as a circular polarizer. According to the experimental results, within the impedance bandwidth of 0.63 GHz from 8.71 to 9.34 GHz, the axial ratio and reflection coefficient S11 of the antenna are less than 3 and −10 dB, respectively. At 9 GHz, the maximum gains of simulation and measurement are 18.5 and 18.3 dB, respectively. The measurement results are according well with the simulation results. Similar methods can be extended to other bands to design high‐gain circularly polarized antennas.</abstract><cop>Hoboken, USA</cop><pub>John Wiley & Sons, Inc</pub><doi>10.1002/mop.32102</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0003-1557-6064</orcidid></addata></record> |
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subjects | antenna chiral metamaterial Circular polarization Fabry‐Perot high‐gain Holes Metamaterials Microstrip antennas partially reflecting surface Polarizers Reflectance |
title | A high‐gain circularly polarized Fabry‐Perot antenna with chiral metamaterial‐based circular polarizer |
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