An Equivalent Circuit Model for Graphene-Based Terahertz Antenna Using the PEEC Method

The electromagnetic (EM) characterization of graphene under general EM environments is becoming of interest in the engineering and scientific research fields. However, its numerical modeling process is extremely cost prohibitive due to the huge contrast between its thickness and other dimensions. In...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:IEEE transactions on antennas and propagation 2016-04, Vol.64 (4), p.1385-1393
Hauptverfasser: Cao, Ying S., Li Jun Jiang, Ruehli, Albert E.
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext bestellen
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 1393
container_issue 4
container_start_page 1385
container_title IEEE transactions on antennas and propagation
container_volume 64
creator Cao, Ying S.
Li Jun Jiang
Ruehli, Albert E.
description The electromagnetic (EM) characterization of graphene under general EM environments is becoming of interest in the engineering and scientific research fields. However, its numerical modeling process is extremely cost prohibitive due to the huge contrast between its thickness and other dimensions. In this work, for the first time, the EM features of graphene are characterized by a circuit model through the partial element equivalent circuit (PEEC) method. The atomically thick graphene is equivalently replaced by an impedance boundary condition. After incorporating the PEEC method, a novel surface conductivity circuit model is derived for graphene. A physical resistor and inductor are added into the conventional PEEC cell due to the dispersive conductivity property of graphene. The proposed novel method significantly reduces the memory and CPU time consumption for general graphene structures when compared with standard numerical finite element method (FEM) or finite difference (FD) methods, where 3-D meshing is unavoidable. This model also transforms the surface conductivity of graphene into a vivid circuit, and physical properties of the material can be conveniently obtained, such as radiation, scattering, and resistance properties, when compared with method of moments (MOM). In addition, the radiation and scattering calculation by MOM entail the cumbersome steps of defining a bounding surface and implementing a multidimensional integrand, while in PEEC, these complications are entirely bypassed by the concise vector-matrix-vector product (VMVP) formulas. To validate the introduced algorithm, various numerical examples are presented and compared with existing references.
doi_str_mv 10.1109/TAP.2016.2521881
format Article
fullrecord <record><control><sourceid>proquest_RIE</sourceid><recordid>TN_cdi_proquest_journals_1787109309</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><ieee_id>7393520</ieee_id><sourcerecordid>4046709081</sourcerecordid><originalsourceid>FETCH-LOGICAL-c291t-fd34a705245647f8e9abe761f29e5cce7bb442d98b2da9daaf0e90715c6b4a4f3</originalsourceid><addsrcrecordid>eNo9kM1LwzAYxoMoOKd3wUvAc2eSJk1zrKVOYcMdNvEW0vaN7ZjplrSC_vV2TIQXHl54PuCH0C0lM0qJelhnqxkjNJkxwWia0jM0oUKkEWOMnqMJITSNFEveL9FVCNvx5SnnE_SWOVwchvbL7MD1OG99NbQ9XnY17LDtPJ57s2_AQfRoAtR4Dd404PsfnLkenDN4E1r3gfsG8KoocryEvunqa3RhzS7AzZ9O0eapWOfP0eJ1_pJni6hiivaRrWNuJBGMi4RLm4IyJciEWqZAVBXIsuSc1SotWW1UbYwloIikokpKbriNp-j-1Lv33WGA0OttN3g3TmoqUzmCicebInJyVb4LwYPVe99-Gv-tKdFHenqkp4_09B-9MXJ3irQA8G-XsYoFI_EvcIFqkA</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>1787109309</pqid></control><display><type>article</type><title>An Equivalent Circuit Model for Graphene-Based Terahertz Antenna Using the PEEC Method</title><source>IEEE Electronic Library (IEL)</source><creator>Cao, Ying S. ; Li Jun Jiang ; Ruehli, Albert E.</creator><creatorcontrib>Cao, Ying S. ; Li Jun Jiang ; Ruehli, Albert E.</creatorcontrib><description>The electromagnetic (EM) characterization of graphene under general EM environments is becoming of interest in the engineering and scientific research fields. However, its numerical modeling process is extremely cost prohibitive due to the huge contrast between its thickness and other dimensions. In this work, for the first time, the EM features of graphene are characterized by a circuit model through the partial element equivalent circuit (PEEC) method. The atomically thick graphene is equivalently replaced by an impedance boundary condition. After incorporating the PEEC method, a novel surface conductivity circuit model is derived for graphene. A physical resistor and inductor are added into the conventional PEEC cell due to the dispersive conductivity property of graphene. The proposed novel method significantly reduces the memory and CPU time consumption for general graphene structures when compared with standard numerical finite element method (FEM) or finite difference (FD) methods, where 3-D meshing is unavoidable. This model also transforms the surface conductivity of graphene into a vivid circuit, and physical properties of the material can be conveniently obtained, such as radiation, scattering, and resistance properties, when compared with method of moments (MOM). In addition, the radiation and scattering calculation by MOM entail the cumbersome steps of defining a bounding surface and implementing a multidimensional integrand, while in PEEC, these complications are entirely bypassed by the concise vector-matrix-vector product (VMVP) formulas. To validate the introduced algorithm, various numerical examples are presented and compared with existing references.</description><identifier>ISSN: 0018-926X</identifier><identifier>EISSN: 1558-2221</identifier><identifier>DOI: 10.1109/TAP.2016.2521881</identifier><identifier>CODEN: IETPAK</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Antennas ; Circuits ; Conductivity ; Graphene ; Impedance ; impedance boundary condition ; Integrated circuit modeling ; Numerical models ; partial element equivalent circuit (PEEC) method ; Simulation ; surface conductivity ; Surface impedance</subject><ispartof>IEEE transactions on antennas and propagation, 2016-04, Vol.64 (4), p.1385-1393</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2016</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c291t-fd34a705245647f8e9abe761f29e5cce7bb442d98b2da9daaf0e90715c6b4a4f3</citedby><cites>FETCH-LOGICAL-c291t-fd34a705245647f8e9abe761f29e5cce7bb442d98b2da9daaf0e90715c6b4a4f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/7393520$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/7393520$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Cao, Ying S.</creatorcontrib><creatorcontrib>Li Jun Jiang</creatorcontrib><creatorcontrib>Ruehli, Albert E.</creatorcontrib><title>An Equivalent Circuit Model for Graphene-Based Terahertz Antenna Using the PEEC Method</title><title>IEEE transactions on antennas and propagation</title><addtitle>TAP</addtitle><description>The electromagnetic (EM) characterization of graphene under general EM environments is becoming of interest in the engineering and scientific research fields. However, its numerical modeling process is extremely cost prohibitive due to the huge contrast between its thickness and other dimensions. In this work, for the first time, the EM features of graphene are characterized by a circuit model through the partial element equivalent circuit (PEEC) method. The atomically thick graphene is equivalently replaced by an impedance boundary condition. After incorporating the PEEC method, a novel surface conductivity circuit model is derived for graphene. A physical resistor and inductor are added into the conventional PEEC cell due to the dispersive conductivity property of graphene. The proposed novel method significantly reduces the memory and CPU time consumption for general graphene structures when compared with standard numerical finite element method (FEM) or finite difference (FD) methods, where 3-D meshing is unavoidable. This model also transforms the surface conductivity of graphene into a vivid circuit, and physical properties of the material can be conveniently obtained, such as radiation, scattering, and resistance properties, when compared with method of moments (MOM). In addition, the radiation and scattering calculation by MOM entail the cumbersome steps of defining a bounding surface and implementing a multidimensional integrand, while in PEEC, these complications are entirely bypassed by the concise vector-matrix-vector product (VMVP) formulas. To validate the introduced algorithm, various numerical examples are presented and compared with existing references.</description><subject>Antennas</subject><subject>Circuits</subject><subject>Conductivity</subject><subject>Graphene</subject><subject>Impedance</subject><subject>impedance boundary condition</subject><subject>Integrated circuit modeling</subject><subject>Numerical models</subject><subject>partial element equivalent circuit (PEEC) method</subject><subject>Simulation</subject><subject>surface conductivity</subject><subject>Surface impedance</subject><issn>0018-926X</issn><issn>1558-2221</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNo9kM1LwzAYxoMoOKd3wUvAc2eSJk1zrKVOYcMdNvEW0vaN7ZjplrSC_vV2TIQXHl54PuCH0C0lM0qJelhnqxkjNJkxwWia0jM0oUKkEWOMnqMJITSNFEveL9FVCNvx5SnnE_SWOVwchvbL7MD1OG99NbQ9XnY17LDtPJ57s2_AQfRoAtR4Dd404PsfnLkenDN4E1r3gfsG8KoocryEvunqa3RhzS7AzZ9O0eapWOfP0eJ1_pJni6hiivaRrWNuJBGMi4RLm4IyJciEWqZAVBXIsuSc1SotWW1UbYwloIikokpKbriNp-j-1Lv33WGA0OttN3g3TmoqUzmCicebInJyVb4LwYPVe99-Gv-tKdFHenqkp4_09B-9MXJ3irQA8G-XsYoFI_EvcIFqkA</recordid><startdate>201604</startdate><enddate>201604</enddate><creator>Cao, Ying S.</creator><creator>Li Jun Jiang</creator><creator>Ruehli, Albert E.</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></search><sort><creationdate>201604</creationdate><title>An Equivalent Circuit Model for Graphene-Based Terahertz Antenna Using the PEEC Method</title><author>Cao, Ying S. ; Li Jun Jiang ; Ruehli, Albert E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c291t-fd34a705245647f8e9abe761f29e5cce7bb442d98b2da9daaf0e90715c6b4a4f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Antennas</topic><topic>Circuits</topic><topic>Conductivity</topic><topic>Graphene</topic><topic>Impedance</topic><topic>impedance boundary condition</topic><topic>Integrated circuit modeling</topic><topic>Numerical models</topic><topic>partial element equivalent circuit (PEEC) method</topic><topic>Simulation</topic><topic>surface conductivity</topic><topic>Surface impedance</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Cao, Ying S.</creatorcontrib><creatorcontrib>Li Jun Jiang</creatorcontrib><creatorcontrib>Ruehli, Albert E.</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 &amp; 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>Cao, Ying S.</au><au>Li Jun Jiang</au><au>Ruehli, Albert E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>An Equivalent Circuit Model for Graphene-Based Terahertz Antenna Using the PEEC Method</atitle><jtitle>IEEE transactions on antennas and propagation</jtitle><stitle>TAP</stitle><date>2016-04</date><risdate>2016</risdate><volume>64</volume><issue>4</issue><spage>1385</spage><epage>1393</epage><pages>1385-1393</pages><issn>0018-926X</issn><eissn>1558-2221</eissn><coden>IETPAK</coden><abstract>The electromagnetic (EM) characterization of graphene under general EM environments is becoming of interest in the engineering and scientific research fields. However, its numerical modeling process is extremely cost prohibitive due to the huge contrast between its thickness and other dimensions. In this work, for the first time, the EM features of graphene are characterized by a circuit model through the partial element equivalent circuit (PEEC) method. The atomically thick graphene is equivalently replaced by an impedance boundary condition. After incorporating the PEEC method, a novel surface conductivity circuit model is derived for graphene. A physical resistor and inductor are added into the conventional PEEC cell due to the dispersive conductivity property of graphene. The proposed novel method significantly reduces the memory and CPU time consumption for general graphene structures when compared with standard numerical finite element method (FEM) or finite difference (FD) methods, where 3-D meshing is unavoidable. This model also transforms the surface conductivity of graphene into a vivid circuit, and physical properties of the material can be conveniently obtained, such as radiation, scattering, and resistance properties, when compared with method of moments (MOM). In addition, the radiation and scattering calculation by MOM entail the cumbersome steps of defining a bounding surface and implementing a multidimensional integrand, while in PEEC, these complications are entirely bypassed by the concise vector-matrix-vector product (VMVP) formulas. To validate the introduced algorithm, various numerical examples are presented and compared with existing references.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TAP.2016.2521881</doi><tpages>9</tpages></addata></record>
fulltext fulltext_linktorsrc
identifier ISSN: 0018-926X
ispartof IEEE transactions on antennas and propagation, 2016-04, Vol.64 (4), p.1385-1393
issn 0018-926X
1558-2221
language eng
recordid cdi_proquest_journals_1787109309
source IEEE Electronic Library (IEL)
subjects Antennas
Circuits
Conductivity
Graphene
Impedance
impedance boundary condition
Integrated circuit modeling
Numerical models
partial element equivalent circuit (PEEC) method
Simulation
surface conductivity
Surface impedance
title An Equivalent Circuit Model for Graphene-Based Terahertz Antenna Using the PEEC Method
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-30T21%3A56%3A06IST&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=An%20Equivalent%20Circuit%20Model%20for%20Graphene-Based%20Terahertz%20Antenna%20Using%20the%20PEEC%20Method&rft.jtitle=IEEE%20transactions%20on%20antennas%20and%20propagation&rft.au=Cao,%20Ying%20S.&rft.date=2016-04&rft.volume=64&rft.issue=4&rft.spage=1385&rft.epage=1393&rft.pages=1385-1393&rft.issn=0018-926X&rft.eissn=1558-2221&rft.coden=IETPAK&rft_id=info:doi/10.1109/TAP.2016.2521881&rft_dat=%3Cproquest_RIE%3E4046709081%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=1787109309&rft_id=info:pmid/&rft_ieee_id=7393520&rfr_iscdi=true