Tuning conductance in C sub(60) devices: defective C sub(60) and endohedral C sub(60) complex
The transport properties and I-V characteristics of C sub(60), defective C sub(60), endohedral C sub(59) complex, and endohedral C sub(60) complex devices have been investigated. The transmission coefficients of the C sub(60) devices have been found to be largely affected by either defect or doping...
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Veröffentlicht in: | Applied physics. A, Materials science & processing Materials science & processing, 2015-02, Vol.118 (2), p.473-477 |
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description | The transport properties and I-V characteristics of C sub(60), defective C sub(60), endohedral C sub(59) complex, and endohedral C sub(60) complex devices have been investigated. The transmission coefficients of the C sub(60) devices have been found to be largely affected by either defect or doping an atom in the center of the C sub(60). The conductance in C sub(60) devices can also be tuned by both defect and doping. In particular, doping an atom into the center of C sub(60) has an obvious effect on tuning conductance. C sub(60), N sub(60), and O sub(60) double the current of the C sub(60) device, while B sub(60) terminates the current at low voltage. |
doi_str_mv | 10.1007/s00339-014-8761-0 |
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The transmission coefficients of the C sub(60) devices have been found to be largely affected by either defect or doping an atom in the center of the C sub(60). The conductance in C sub(60) devices can also be tuned by both defect and doping. In particular, doping an atom into the center of C sub(60) has an obvious effect on tuning conductance. C sub(60), N sub(60), and O sub(60) double the current of the C sub(60) device, while B sub(60) terminates the current at low voltage.</description><identifier>ISSN: 0947-8396</identifier><identifier>EISSN: 1432-0630</identifier><identifier>DOI: 10.1007/s00339-014-8761-0</identifier><language>eng</language><subject>Buckminsterfullerene ; Conductance ; Defects ; Devices ; Doping ; Fullerenes ; Transport properties ; Tuning</subject><ispartof>Applied physics. 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The conductance in C sub(60) devices can also be tuned by both defect and doping. In particular, doping an atom into the center of C sub(60) has an obvious effect on tuning conductance. C sub(60), N sub(60), and O sub(60) double the current of the C sub(60) device, while B sub(60) terminates the current at low voltage.</description><subject>Buckminsterfullerene</subject><subject>Conductance</subject><subject>Defects</subject><subject>Devices</subject><subject>Doping</subject><subject>Fullerenes</subject><subject>Transport properties</subject><subject>Tuning</subject><issn>0947-8396</issn><issn>1432-0630</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqVisFOAyEURYnRxLH1A9yxrAvsYyDAuG00fkC3pqHwqhgGxr6h8fPtwkW33s05ybmMPUh4kgB2TQBKDQKkFs4aKeCKdVKrXoBRcM06GLQVTg3mlt0RfcF5uu879r5tJZUPHmqJLcy-BOSp8A2ntl8ZeOQRTykgPZ_lgGFOJ7yIvkSOJdZPjEefL0Ko45TxZ8luDj4T3v9xwVavL9vNm5iO9bshzbsxUcCcfcHaaCeNGZzVzln1j-svUOpLMA</recordid><startdate>20150201</startdate><enddate>20150201</enddate><creator>Li, Guiqin</creator><scope>7TB</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20150201</creationdate><title>Tuning conductance in C sub(60) devices: defective C sub(60) and endohedral C sub(60) complex</title><author>Li, Guiqin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_16698748873</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Buckminsterfullerene</topic><topic>Conductance</topic><topic>Defects</topic><topic>Devices</topic><topic>Doping</topic><topic>Fullerenes</topic><topic>Transport properties</topic><topic>Tuning</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Li, Guiqin</creatorcontrib><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Applied physics. A, Materials science & processing</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Li, Guiqin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Tuning conductance in C sub(60) devices: defective C sub(60) and endohedral C sub(60) complex</atitle><jtitle>Applied physics. A, Materials science & processing</jtitle><date>2015-02-01</date><risdate>2015</risdate><volume>118</volume><issue>2</issue><spage>473</spage><epage>477</epage><pages>473-477</pages><issn>0947-8396</issn><eissn>1432-0630</eissn><abstract>The transport properties and I-V characteristics of C sub(60), defective C sub(60), endohedral C sub(59) complex, and endohedral C sub(60) complex devices have been investigated. The transmission coefficients of the C sub(60) devices have been found to be largely affected by either defect or doping an atom in the center of the C sub(60). The conductance in C sub(60) devices can also be tuned by both defect and doping. In particular, doping an atom into the center of C sub(60) has an obvious effect on tuning conductance. C sub(60), N sub(60), and O sub(60) double the current of the C sub(60) device, while B sub(60) terminates the current at low voltage.</abstract><doi>10.1007/s00339-014-8761-0</doi></addata></record> |
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subjects | Buckminsterfullerene Conductance Defects Devices Doping Fullerenes Transport properties Tuning |
title | Tuning conductance in C sub(60) devices: defective C sub(60) and endohedral C sub(60) complex |
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