Complementary Metasurfaces for Guiding Electromagnetic Wave
Metasurfaces can be employed for designing waveguides that confine the electromagnetic energy while they are open structures. In this communication, we introduce a new type of such waveguides, formed by two penetrable metasurfaces having complementary isotropic surface impedances. We theoretically s...
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Veröffentlicht in: | IEEE transactions on antennas and propagation 2021-03, Vol.69 (3), p.1815-1820 |
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creator | Ma, X. Mirmoosa, M. S. Tretyakov, S. A. |
description | Metasurfaces can be employed for designing waveguides that confine the electromagnetic energy while they are open structures. In this communication, we introduce a new type of such waveguides, formed by two penetrable metasurfaces having complementary isotropic surface impedances. We theoretically study the guided modes supported by the proposed structure and discuss the corresponding dispersion properties. We show the results for different scenarios in which the surface impedances possess nonresonant or resonant characteristics, and the distance between the two metasurfaces changes from large values to the extreme limit of zero. We also derive and describe the general condition for existence of two modes with orthogonal polarizations having the same phase velocity. In the particular case in which the metasurfaces are complementary and the distance between them is not small, we indicate that such phenomenon occurs within a broad frequency range. This property can be promising for applications in leaky-wave antennas and field focusing. |
doi_str_mv | 10.1109/TAP.2020.3018536 |
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S. ; Tretyakov, S. A.</creator><creatorcontrib>Ma, X. ; Mirmoosa, M. S. ; Tretyakov, S. A.</creatorcontrib><description>Metasurfaces can be employed for designing waveguides that confine the electromagnetic energy while they are open structures. In this communication, we introduce a new type of such waveguides, formed by two penetrable metasurfaces having complementary isotropic surface impedances. We theoretically study the guided modes supported by the proposed structure and discuss the corresponding dispersion properties. We show the results for different scenarios in which the surface impedances possess nonresonant or resonant characteristics, and the distance between the two metasurfaces changes from large values to the extreme limit of zero. We also derive and describe the general condition for existence of two modes with orthogonal polarizations having the same phase velocity. In the particular case in which the metasurfaces are complementary and the distance between them is not small, we indicate that such phenomenon occurs within a broad frequency range. This property can be promising for applications in leaky-wave antennas and field focusing.</description><identifier>ISSN: 0018-926X</identifier><identifier>EISSN: 1558-2221</identifier><identifier>DOI: 10.1109/TAP.2020.3018536</identifier><identifier>CODEN: IETPAK</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Complementary metasurfaces ; Dispersion ; dispersion curve ; Electromagnetic radiation ; Extreme values ; Frequency ranges ; Impedance ; Leaky waves ; Metasurfaces ; open waveguides ; Phase velocity ; Planar waveguides ; Resonant frequency ; Surface impedance ; Surface waves ; Waveguides</subject><ispartof>IEEE transactions on antennas and propagation, 2021-03, Vol.69 (3), p.1815-1820</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2021</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c333t-efbb86a45ceedc48d6498bf786dfc3ea1224cc9879b534bbe7137062eb7754123</citedby><cites>FETCH-LOGICAL-c333t-efbb86a45ceedc48d6498bf786dfc3ea1224cc9879b534bbe7137062eb7754123</cites><orcidid>0000-0001-9629-1380 ; 0000-0002-4989-7651 ; 0000-0002-4738-9987</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/9179000$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27923,27924,54757</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/9179000$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Ma, X.</creatorcontrib><creatorcontrib>Mirmoosa, M. S.</creatorcontrib><creatorcontrib>Tretyakov, S. A.</creatorcontrib><title>Complementary Metasurfaces for Guiding Electromagnetic Wave</title><title>IEEE transactions on antennas and propagation</title><addtitle>TAP</addtitle><description>Metasurfaces can be employed for designing waveguides that confine the electromagnetic energy while they are open structures. In this communication, we introduce a new type of such waveguides, formed by two penetrable metasurfaces having complementary isotropic surface impedances. We theoretically study the guided modes supported by the proposed structure and discuss the corresponding dispersion properties. We show the results for different scenarios in which the surface impedances possess nonresonant or resonant characteristics, and the distance between the two metasurfaces changes from large values to the extreme limit of zero. We also derive and describe the general condition for existence of two modes with orthogonal polarizations having the same phase velocity. In the particular case in which the metasurfaces are complementary and the distance between them is not small, we indicate that such phenomenon occurs within a broad frequency range. This property can be promising for applications in leaky-wave antennas and field focusing.</description><subject>Complementary metasurfaces</subject><subject>Dispersion</subject><subject>dispersion curve</subject><subject>Electromagnetic radiation</subject><subject>Extreme values</subject><subject>Frequency ranges</subject><subject>Impedance</subject><subject>Leaky waves</subject><subject>Metasurfaces</subject><subject>open waveguides</subject><subject>Phase velocity</subject><subject>Planar waveguides</subject><subject>Resonant frequency</subject><subject>Surface impedance</subject><subject>Surface waves</subject><subject>Waveguides</subject><issn>0018-926X</issn><issn>1558-2221</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNo9kM1LAzEQxYMoWKt3wcuC513zuZvgqZRahYoeKnoLSXZStnR3a7Ir-N-b0uJpmOG9N7wfQrcEF4Rg9bCevRcUU1wwTKRg5RmaECFkTikl52iC0zVXtPy6RFcxbtPKJecT9Djv2_0OWugGE36zVxhMHIM3DmLm-5Atx6Zuuk222IEbQt-aTQdD47JP8wPX6MKbXYSb05yij6fFev6cr96WL_PZKneMsSEHb60sDRcOoHZc1iVX0vpKlrV3DAyhlDunZKWsYNxaqAircEnBVpXghLIpuj_m7kP_PUIc9LYfQ5deapqiSomJkEmFjyoX-hgDeL0PTZtKaYL1AZFOiPQBkT4hSpa7o6UBgH-5IpXCGLM_WoVh_g</recordid><startdate>20210301</startdate><enddate>20210301</enddate><creator>Ma, X.</creator><creator>Mirmoosa, M. S.</creator><creator>Tretyakov, S. A.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-9629-1380</orcidid><orcidid>https://orcid.org/0000-0002-4989-7651</orcidid><orcidid>https://orcid.org/0000-0002-4738-9987</orcidid></search><sort><creationdate>20210301</creationdate><title>Complementary Metasurfaces for Guiding Electromagnetic Wave</title><author>Ma, X. ; Mirmoosa, M. S. ; Tretyakov, S. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c333t-efbb86a45ceedc48d6498bf786dfc3ea1224cc9879b534bbe7137062eb7754123</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Complementary metasurfaces</topic><topic>Dispersion</topic><topic>dispersion curve</topic><topic>Electromagnetic radiation</topic><topic>Extreme values</topic><topic>Frequency ranges</topic><topic>Impedance</topic><topic>Leaky waves</topic><topic>Metasurfaces</topic><topic>open waveguides</topic><topic>Phase velocity</topic><topic>Planar waveguides</topic><topic>Resonant frequency</topic><topic>Surface impedance</topic><topic>Surface waves</topic><topic>Waveguides</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ma, X.</creatorcontrib><creatorcontrib>Mirmoosa, M. S.</creatorcontrib><creatorcontrib>Tretyakov, S. A.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><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_linktorsrc</fulltext></delivery><addata><au>Ma, X.</au><au>Mirmoosa, M. S.</au><au>Tretyakov, S. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Complementary Metasurfaces for Guiding Electromagnetic Wave</atitle><jtitle>IEEE transactions on antennas and propagation</jtitle><stitle>TAP</stitle><date>2021-03-01</date><risdate>2021</risdate><volume>69</volume><issue>3</issue><spage>1815</spage><epage>1820</epage><pages>1815-1820</pages><issn>0018-926X</issn><eissn>1558-2221</eissn><coden>IETPAK</coden><abstract>Metasurfaces can be employed for designing waveguides that confine the electromagnetic energy while they are open structures. In this communication, we introduce a new type of such waveguides, formed by two penetrable metasurfaces having complementary isotropic surface impedances. We theoretically study the guided modes supported by the proposed structure and discuss the corresponding dispersion properties. We show the results for different scenarios in which the surface impedances possess nonresonant or resonant characteristics, and the distance between the two metasurfaces changes from large values to the extreme limit of zero. We also derive and describe the general condition for existence of two modes with orthogonal polarizations having the same phase velocity. In the particular case in which the metasurfaces are complementary and the distance between them is not small, we indicate that such phenomenon occurs within a broad frequency range. This property can be promising for applications in leaky-wave antennas and field focusing.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TAP.2020.3018536</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0001-9629-1380</orcidid><orcidid>https://orcid.org/0000-0002-4989-7651</orcidid><orcidid>https://orcid.org/0000-0002-4738-9987</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Complementary metasurfaces Dispersion dispersion curve Electromagnetic radiation Extreme values Frequency ranges Impedance Leaky waves Metasurfaces open waveguides Phase velocity Planar waveguides Resonant frequency Surface impedance Surface waves Waveguides |
title | Complementary Metasurfaces for Guiding Electromagnetic Wave |
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