Observation of negative contact resistances in graphene field-effect transistors
The gate-voltage ( V G ) dependence of the contact resistance ( R C ) in graphene field-effect transistors is characterized by the transmission line model. The R C - V G characteristics of Ag, Cu, and Au contacts display a dip around the charge neutrality point and become even negative with Ag conta...
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Veröffentlicht in: | Journal of applied physics 2012-04, Vol.111 (8), p.084314-084314-7 |
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container_title | Journal of applied physics |
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creator | Nouchi, Ryo Saito, Tatsuya Tanigaki, Katsumi |
description | The gate-voltage (
V
G
) dependence of the contact resistance (
R
C
) in graphene field-effect transistors is characterized by the transmission line model. The
R
C
-
V
G
characteristics of Ag, Cu, and Au contacts display a dip around the charge neutrality point and become even negative with Ag contacts. The dip structure is well reproduced by a model calculation that considers a metal-contact-induced potential variation near the metal contact edges. The apparently negative
R
C
originates with the carrier doping from the metal contacts to the graphene channel and appears when the doping effect is more substantial than the actual contact resistance precisely at the contacts. The negative
R
C
can appear at the metal contacts to Dirac-cone systems such as graphene. |
doi_str_mv | 10.1063/1.4705367 |
format | Article |
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V
G
) dependence of the contact resistance (
R
C
) in graphene field-effect transistors is characterized by the transmission line model. The
R
C
-
V
G
characteristics of Ag, Cu, and Au contacts display a dip around the charge neutrality point and become even negative with Ag contacts. The dip structure is well reproduced by a model calculation that considers a metal-contact-induced potential variation near the metal contact edges. The apparently negative
R
C
originates with the carrier doping from the metal contacts to the graphene channel and appears when the doping effect is more substantial than the actual contact resistance precisely at the contacts. The negative
R
C
can appear at the metal contacts to Dirac-cone systems such as graphene.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.4705367</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>American Institute of Physics</publisher><subject>Contact ; Contact resistance ; Dipping ; Graphene ; Reinforced concrete ; Semiconductor devices ; Silver ; Transistors</subject><ispartof>Journal of applied physics, 2012-04, Vol.111 (8), p.084314-084314-7</ispartof><rights>2012 American Institute of Physics</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c418t-881b3d81e7f4ffb62068f8b3c385f1b9da4bfb48207835f69e6605538e9a73a53</citedby><cites>FETCH-LOGICAL-c418t-881b3d81e7f4ffb62068f8b3c385f1b9da4bfb48207835f69e6605538e9a73a53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jap/article-lookup/doi/10.1063/1.4705367$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,1559,4512,27924,27925,76384,76390</link.rule.ids></links><search><creatorcontrib>Nouchi, Ryo</creatorcontrib><creatorcontrib>Saito, Tatsuya</creatorcontrib><creatorcontrib>Tanigaki, Katsumi</creatorcontrib><title>Observation of negative contact resistances in graphene field-effect transistors</title><title>Journal of applied physics</title><description>The gate-voltage (
V
G
) dependence of the contact resistance (
R
C
) in graphene field-effect transistors is characterized by the transmission line model. The
R
C
-
V
G
characteristics of Ag, Cu, and Au contacts display a dip around the charge neutrality point and become even negative with Ag contacts. The dip structure is well reproduced by a model calculation that considers a metal-contact-induced potential variation near the metal contact edges. The apparently negative
R
C
originates with the carrier doping from the metal contacts to the graphene channel and appears when the doping effect is more substantial than the actual contact resistance precisely at the contacts. The negative
R
C
can appear at the metal contacts to Dirac-cone systems such as graphene.</description><subject>Contact</subject><subject>Contact resistance</subject><subject>Dipping</subject><subject>Graphene</subject><subject>Reinforced concrete</subject><subject>Semiconductor devices</subject><subject>Silver</subject><subject>Transistors</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNp10DtPwzAUhmELgUQpDPyDjDCk-MRxYi9IqOImVSoDzJbtHpeg1C62W4l_T3oZWJjOGR59w0vINdAJ0IbdwaRuKWdNe0JGQIUsW87pKRlRWkEpZCvPyUVKX5QCCCZH5G1uEsatzl3wRXCFx-Xwb7GwwWdtcxExdSlrbzEVnS-WUa8_0WPhOuwXJTqHA8pR-x0LMV2SM6f7hFfHOyYfT4_v05dyNn9-nT7MSluDyKUQYNhCALauds40FW2EE4ZZJrgDIxe6Ns7UoqKtYNw1EpuGcs4ESt0yzdmY3Bx21zF8bzBlteqSxb7XHsMmKWAVq4BKWg309kBtDClFdGodu5WOPwqo2lVToI7VBnt_sMl2eV_lf_wnnQpO7dOxX1uxdPg</recordid><startdate>20120415</startdate><enddate>20120415</enddate><creator>Nouchi, Ryo</creator><creator>Saito, Tatsuya</creator><creator>Tanigaki, Katsumi</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20120415</creationdate><title>Observation of negative contact resistances in graphene field-effect transistors</title><author>Nouchi, Ryo ; Saito, Tatsuya ; Tanigaki, Katsumi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c418t-881b3d81e7f4ffb62068f8b3c385f1b9da4bfb48207835f69e6605538e9a73a53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Contact</topic><topic>Contact resistance</topic><topic>Dipping</topic><topic>Graphene</topic><topic>Reinforced concrete</topic><topic>Semiconductor devices</topic><topic>Silver</topic><topic>Transistors</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nouchi, Ryo</creatorcontrib><creatorcontrib>Saito, Tatsuya</creatorcontrib><creatorcontrib>Tanigaki, Katsumi</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nouchi, Ryo</au><au>Saito, Tatsuya</au><au>Tanigaki, Katsumi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Observation of negative contact resistances in graphene field-effect transistors</atitle><jtitle>Journal of applied physics</jtitle><date>2012-04-15</date><risdate>2012</risdate><volume>111</volume><issue>8</issue><spage>084314</spage><epage>084314-7</epage><pages>084314-084314-7</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>The gate-voltage (
V
G
) dependence of the contact resistance (
R
C
) in graphene field-effect transistors is characterized by the transmission line model. The
R
C
-
V
G
characteristics of Ag, Cu, and Au contacts display a dip around the charge neutrality point and become even negative with Ag contacts. The dip structure is well reproduced by a model calculation that considers a metal-contact-induced potential variation near the metal contact edges. The apparently negative
R
C
originates with the carrier doping from the metal contacts to the graphene channel and appears when the doping effect is more substantial than the actual contact resistance precisely at the contacts. The negative
R
C
can appear at the metal contacts to Dirac-cone systems such as graphene.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.4705367</doi><oa>free_for_read</oa></addata></record> |
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language | eng |
recordid | cdi_proquest_miscellaneous_1323210902 |
source | AIP Journals Complete; AIP Digital Archive; Alma/SFX Local Collection |
subjects | Contact Contact resistance Dipping Graphene Reinforced concrete Semiconductor devices Silver Transistors |
title | Observation of negative contact resistances in graphene field-effect transistors |
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