Dispersivity of Balanced Near-Zero Permittivity and Permeability (EMNZ) Medium
ε-near-zero (ENZ), μ-near-zero (MNZ), and ε-and-μ-near-zero (EMNZ) materials all exhibit the property of n = √(ε r μ r ) ≈ 0. The wave impedance Z = (μ/ε) 1/2 , though, is different for the different materials. For the EMNZ, the impedance can remain finite, in contrast to the ENZ and MNZ materials....
Gespeichert in:
| Veröffentlicht in: | IEEE transactions on microwave theory and techniques 2016-10, Vol.64 (10), p.3108-3112 |
|---|---|
| 1. Verfasser: | |
| Format: | Artikel |
| Sprache: | eng |
| Schlagworte: | |
| Online-Zugang: | Volltext bestellen |
| Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
| container_end_page | 3112 |
|---|---|
| container_issue | 10 |
| container_start_page | 3108 |
| container_title | IEEE transactions on microwave theory and techniques |
| container_volume | 64 |
| creator | Kastner, Raphael |
| description | ε-near-zero (ENZ), μ-near-zero (MNZ), and ε-and-μ-near-zero (EMNZ) materials all exhibit the property of n = √(ε r μ r ) ≈ 0. The wave impedance Z = (μ/ε) 1/2 , though, is different for the different materials. For the EMNZ, the impedance can remain finite, in contrast to the ENZ and MNZ materials. Therefore, the electric and magnetic fields within the EMNZ can remain coupled, unlike the ENZ and MNZ. This paper presents an analysis of dispersivity in an EMNZ layer under the condition of balance μ r = ε r . One possible application for this condition is seen in the analysis of transmission and reflection from an EMNZ-free space interface, which reveals that a perfect match condition is possible for normal incidence, while for any other incidence angle, this interface is a perfect reflector. |
| doi_str_mv | 10.1109/TMTT.2016.2599159 |
| format | Article |
| fullrecord | <record><control><sourceid>proquest_RIE</sourceid><recordid>TN_cdi_ieee_primary_7549113</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><ieee_id>7549113</ieee_id><sourcerecordid>4223961371</sourcerecordid><originalsourceid>FETCH-LOGICAL-c293t-26354edc3c14da64811751c615d1cdfc374ae146c69bfaa84d9a05048aff901b3</originalsourceid><addsrcrecordid>eNo9kD1PwzAQhi0EEqXwAxBLJBYYUnyxncQjlPIhtYUhLF0s1z5Lrtqm2ClS_z0JqZhO9-p576SHkGugIwAqH6pZVY0yCvkoE1KCkCdkAEIUqcwLekoGlEKZSl7Sc3IR46pduaDlgMyffdxhiP7HN4ekdsmTXuutQZvMUYd0gaFOPjFsfNP0iN7avwD10q-74G4ymy_ukxlav99ckjOn1xGvjnNIvl4m1fgtnX68vo8fp6nJJGvSLGeCozXMALc65yVAIcDkICwY6wwruEbgucnl0mldcis1FZSX2jlJYcmG5La_uwv19x5jo1b1PmzblwpKBpTKTBQtBT1lQh1jQKd2wW90OCigqtOmOm2q06aO2trOTd_xiPjPF4JLAMZ-AcEcaFI</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>1831009257</pqid></control><display><type>article</type><title>Dispersivity of Balanced Near-Zero Permittivity and Permeability (EMNZ) Medium</title><source>IEEE Electronic Library (IEL)</source><creator>Kastner, Raphael</creator><creatorcontrib>Kastner, Raphael</creatorcontrib><description>ε-near-zero (ENZ), μ-near-zero (MNZ), and ε-and-μ-near-zero (EMNZ) materials all exhibit the property of n = √(ε r μ r ) ≈ 0. The wave impedance Z = (μ/ε) 1/2 , though, is different for the different materials. For the EMNZ, the impedance can remain finite, in contrast to the ENZ and MNZ materials. Therefore, the electric and magnetic fields within the EMNZ can remain coupled, unlike the ENZ and MNZ. This paper presents an analysis of dispersivity in an EMNZ layer under the condition of balance μ r = ε r . One possible application for this condition is seen in the analysis of transmission and reflection from an EMNZ-free space interface, which reveals that a perfect match condition is possible for normal incidence, while for any other incidence angle, this interface is a perfect reflector.</description><identifier>ISSN: 0018-9480</identifier><identifier>EISSN: 1557-9670</identifier><identifier>DOI: 10.1109/TMTT.2016.2599159</identifier><identifier>CODEN: IETMAB</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>epsilon -near-zero (EMZ) ; Impedance ; Media ; Microwave theory and techniques ; mu -near-zero (MNZ) ; perfectly matched surface ; Permeability ; Permittivity ; Surface impedance ; Surface waves</subject><ispartof>IEEE transactions on microwave theory and techniques, 2016-10, Vol.64 (10), p.3108-3112</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2016</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c293t-26354edc3c14da64811751c615d1cdfc374ae146c69bfaa84d9a05048aff901b3</citedby><cites>FETCH-LOGICAL-c293t-26354edc3c14da64811751c615d1cdfc374ae146c69bfaa84d9a05048aff901b3</cites><orcidid>0000-0001-7092-0708</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/7549113$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,776,780,792,27901,27902,54733</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/7549113$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Kastner, Raphael</creatorcontrib><title>Dispersivity of Balanced Near-Zero Permittivity and Permeability (EMNZ) Medium</title><title>IEEE transactions on microwave theory and techniques</title><addtitle>TMTT</addtitle><description>ε-near-zero (ENZ), μ-near-zero (MNZ), and ε-and-μ-near-zero (EMNZ) materials all exhibit the property of n = √(ε r μ r ) ≈ 0. The wave impedance Z = (μ/ε) 1/2 , though, is different for the different materials. For the EMNZ, the impedance can remain finite, in contrast to the ENZ and MNZ materials. Therefore, the electric and magnetic fields within the EMNZ can remain coupled, unlike the ENZ and MNZ. This paper presents an analysis of dispersivity in an EMNZ layer under the condition of balance μ r = ε r . One possible application for this condition is seen in the analysis of transmission and reflection from an EMNZ-free space interface, which reveals that a perfect match condition is possible for normal incidence, while for any other incidence angle, this interface is a perfect reflector.</description><subject>epsilon -near-zero (EMZ)</subject><subject>Impedance</subject><subject>Media</subject><subject>Microwave theory and techniques</subject><subject>mu -near-zero (MNZ)</subject><subject>perfectly matched surface</subject><subject>Permeability</subject><subject>Permittivity</subject><subject>Surface impedance</subject><subject>Surface waves</subject><issn>0018-9480</issn><issn>1557-9670</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNo9kD1PwzAQhi0EEqXwAxBLJBYYUnyxncQjlPIhtYUhLF0s1z5Lrtqm2ClS_z0JqZhO9-p576SHkGugIwAqH6pZVY0yCvkoE1KCkCdkAEIUqcwLekoGlEKZSl7Sc3IR46pduaDlgMyffdxhiP7HN4ekdsmTXuutQZvMUYd0gaFOPjFsfNP0iN7avwD10q-74G4ymy_ukxlav99ckjOn1xGvjnNIvl4m1fgtnX68vo8fp6nJJGvSLGeCozXMALc65yVAIcDkICwY6wwruEbgucnl0mldcis1FZSX2jlJYcmG5La_uwv19x5jo1b1PmzblwpKBpTKTBQtBT1lQh1jQKd2wW90OCigqtOmOm2q06aO2trOTd_xiPjPF4JLAMZ-AcEcaFI</recordid><startdate>201610</startdate><enddate>201610</enddate><creator>Kastner, Raphael</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/0000-0001-7092-0708</orcidid></search><sort><creationdate>201610</creationdate><title>Dispersivity of Balanced Near-Zero Permittivity and Permeability (EMNZ) Medium</title><author>Kastner, Raphael</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c293t-26354edc3c14da64811751c615d1cdfc374ae146c69bfaa84d9a05048aff901b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>epsilon -near-zero (EMZ)</topic><topic>Impedance</topic><topic>Media</topic><topic>Microwave theory and techniques</topic><topic>mu -near-zero (MNZ)</topic><topic>perfectly matched surface</topic><topic>Permeability</topic><topic>Permittivity</topic><topic>Surface impedance</topic><topic>Surface waves</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kastner, Raphael</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 microwave theory and techniques</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Kastner, Raphael</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dispersivity of Balanced Near-Zero Permittivity and Permeability (EMNZ) Medium</atitle><jtitle>IEEE transactions on microwave theory and techniques</jtitle><stitle>TMTT</stitle><date>2016-10</date><risdate>2016</risdate><volume>64</volume><issue>10</issue><spage>3108</spage><epage>3112</epage><pages>3108-3112</pages><issn>0018-9480</issn><eissn>1557-9670</eissn><coden>IETMAB</coden><abstract>ε-near-zero (ENZ), μ-near-zero (MNZ), and ε-and-μ-near-zero (EMNZ) materials all exhibit the property of n = √(ε r μ r ) ≈ 0. The wave impedance Z = (μ/ε) 1/2 , though, is different for the different materials. For the EMNZ, the impedance can remain finite, in contrast to the ENZ and MNZ materials. Therefore, the electric and magnetic fields within the EMNZ can remain coupled, unlike the ENZ and MNZ. This paper presents an analysis of dispersivity in an EMNZ layer under the condition of balance μ r = ε r . One possible application for this condition is seen in the analysis of transmission and reflection from an EMNZ-free space interface, which reveals that a perfect match condition is possible for normal incidence, while for any other incidence angle, this interface is a perfect reflector.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TMTT.2016.2599159</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0001-7092-0708</orcidid></addata></record> |
| fulltext | fulltext_linktorsrc |
| identifier | ISSN: 0018-9480 |
| ispartof | IEEE transactions on microwave theory and techniques, 2016-10, Vol.64 (10), p.3108-3112 |
| issn | 0018-9480 1557-9670 |
| language | eng |
| recordid | cdi_ieee_primary_7549113 |
| source | IEEE Electronic Library (IEL) |
| subjects | epsilon -near-zero (EMZ) Impedance Media Microwave theory and techniques mu -near-zero (MNZ) perfectly matched surface Permeability Permittivity Surface impedance Surface waves |
| title | Dispersivity of Balanced Near-Zero Permittivity and Permeability (EMNZ) Medium |
| url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-06T21%3A05%3A59IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_RIE&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Dispersivity%20of%20Balanced%20Near-Zero%20Permittivity%20and%20Permeability%20(EMNZ)%20Medium&rft.jtitle=IEEE%20transactions%20on%20microwave%20theory%20and%20techniques&rft.au=Kastner,%20Raphael&rft.date=2016-10&rft.volume=64&rft.issue=10&rft.spage=3108&rft.epage=3112&rft.pages=3108-3112&rft.issn=0018-9480&rft.eissn=1557-9670&rft.coden=IETMAB&rft_id=info:doi/10.1109/TMTT.2016.2599159&rft_dat=%3Cproquest_RIE%3E4223961371%3C/proquest_RIE%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=1831009257&rft_id=info:pmid/&rft_ieee_id=7549113&rfr_iscdi=true |