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Patterned Partially Hydrogenated Graphene (C4H) and Its One-Dimensional Analogues: A Computational Study
By means of density functional theory (DFT) computations, we systematically studied the structural and electronic properties of the experimentally just achieved new two-dimensional (2D) hydrocarbon the patterned partially hydrogenated graphene with formula C4H ( Adv. Mater 2011, 23, 4497 ), and in...
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Published in: | Journal of physical chemistry. C 2012-02, Vol.116 (7), p.4526-4534 |
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container_title | Journal of physical chemistry. C |
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creator | Li, Yafei Chen, Zhongfang |
description | By means of density functional theory (DFT) computations, we systematically studied the structural and electronic properties of the experimentally just achieved new two-dimensional (2D) hydrocarbon the patterned partially hydrogenated graphene with formula C4H ( Adv. Mater 2011, 23, 4497 ), and in particular its one-dimensional (1D) analogues. The C4H layer is a stable 2D crystal featured with periodic Clar sextet aromatic rings and is semiconducting with a wide band gap; however, this single-sided patterned partially hydrogenated C4H layer can only be obtained when the possibility of double-sided hydrogenation is excluded, since the double-sided graphane-embedded structure is energetically more favorable. The 1D C4H nanotubes, rolled up by the C4H layer, exhibit excellent thermodynamic properties and all have a wide band gap regardless of the tube diameter and chirality. In contrast, cutting the C4H layer into 1D C4H nanoribbons can result in rich electronic characteristics: they can be metallic or semiconducting depending on the chirality and edge configuration. |
doi_str_mv | 10.1021/jp212499h |
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Mater 2011, 23, 4497 ), and in particular its one-dimensional (1D) analogues. The C4H layer is a stable 2D crystal featured with periodic Clar sextet aromatic rings and is semiconducting with a wide band gap; however, this single-sided patterned partially hydrogenated C4H layer can only be obtained when the possibility of double-sided hydrogenation is excluded, since the double-sided graphane-embedded structure is energetically more favorable. The 1D C4H nanotubes, rolled up by the C4H layer, exhibit excellent thermodynamic properties and all have a wide band gap regardless of the tube diameter and chirality. In contrast, cutting the C4H layer into 1D C4H nanoribbons can result in rich electronic characteristics: they can be metallic or semiconducting depending on the chirality and edge configuration.</description><identifier>ISSN: 1932-7447</identifier><identifier>EISSN: 1932-7455</identifier><identifier>DOI: 10.1021/jp212499h</identifier><language>eng</language><publisher>Columbus, OH: American Chemical Society</publisher><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Cross-disciplinary physics: materials science; rheology ; Electron states ; Electron states and collective excitations in thin films, multilayers, quantum wells, mesoscopic and nanoscale systems ; Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures ; Exact sciences and technology ; Fullerenes and related materials; diamonds, graphite ; Materials science ; Methods of electronic structure calculations ; Nanoscale materials and structures: fabrication and characterization ; Nanotubes ; Physics ; Specific materials</subject><ispartof>Journal of physical chemistry. 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In contrast, cutting the C4H layer into 1D C4H nanoribbons can result in rich electronic characteristics: they can be metallic or semiconducting depending on the chirality and edge configuration.</description><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Electron states</subject><subject>Electron states and collective excitations in thin films, multilayers, quantum wells, mesoscopic and nanoscale systems</subject><subject>Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures</subject><subject>Exact sciences and technology</subject><subject>Fullerenes and related materials; diamonds, graphite</subject><subject>Materials science</subject><subject>Methods of electronic structure calculations</subject><subject>Nanoscale materials and structures: fabrication and characterization</subject><subject>Nanotubes</subject><subject>Physics</subject><subject>Specific materials</subject><issn>1932-7447</issn><issn>1932-7455</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNptkDFPwzAQhS0EEqUw8A-8INEhYDt2nLBVAdpKlVoJmKNrbLepUieynSH_nqCgsrDcnd69e9J9CN1T8kQJo8_HllHGs-xwgSY0i1kkuRCX55nLa3Tj_ZEQERMaT9BhCyFoZ7XCW3Chgrru8bJXrtlrC2GQFw7ag7YaP-Z8OcNgFV4FjzdWR6_VSVtfNRZqPB9Ks--0f8FznDentgsQxtVH6FR_i64M1F7f_fYp-np_-8yX0XqzWOXzdQQszUKkJE1inmgjqBLxLtWGm1gTkrIdZaSk3LCEiJSWFEymdGqkEZJTrkrGU-AinqLZmFu6xnunTdG66gSuLygpfhAVZ0SD92H0tuBLqI0DW1b-fMCETAZs8s8HpS-OTeeGr_w_ed_IjHHZ</recordid><startdate>20120223</startdate><enddate>20120223</enddate><creator>Li, Yafei</creator><creator>Chen, Zhongfang</creator><general>American Chemical Society</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20120223</creationdate><title>Patterned Partially Hydrogenated Graphene (C4H) and Its One-Dimensional Analogues: A Computational Study</title><author>Li, Yafei ; Chen, Zhongfang</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a289t-d716346ef51d53b8ef4f3e0082b120c14f260581c1af9de8f7f57414dc248a453</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Electron states</topic><topic>Electron states and collective excitations in thin films, multilayers, quantum wells, mesoscopic and nanoscale systems</topic><topic>Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures</topic><topic>Exact sciences and technology</topic><topic>Fullerenes and related materials; diamonds, graphite</topic><topic>Materials science</topic><topic>Methods of electronic structure calculations</topic><topic>Nanoscale materials and structures: fabrication and characterization</topic><topic>Nanotubes</topic><topic>Physics</topic><topic>Specific materials</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Li, Yafei</creatorcontrib><creatorcontrib>Chen, Zhongfang</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Journal of physical chemistry. C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Li, Yafei</au><au>Chen, Zhongfang</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Patterned Partially Hydrogenated Graphene (C4H) and Its One-Dimensional Analogues: A Computational Study</atitle><jtitle>Journal of physical chemistry. C</jtitle><addtitle>J. Phys. Chem. C</addtitle><date>2012-02-23</date><risdate>2012</risdate><volume>116</volume><issue>7</issue><spage>4526</spage><epage>4534</epage><pages>4526-4534</pages><issn>1932-7447</issn><eissn>1932-7455</eissn><abstract>By means of density functional theory (DFT) computations, we systematically studied the structural and electronic properties of the experimentally just achieved new two-dimensional (2D) hydrocarbon the patterned partially hydrogenated graphene with formula C4H ( Adv. Mater 2011, 23, 4497 ), and in particular its one-dimensional (1D) analogues. The C4H layer is a stable 2D crystal featured with periodic Clar sextet aromatic rings and is semiconducting with a wide band gap; however, this single-sided patterned partially hydrogenated C4H layer can only be obtained when the possibility of double-sided hydrogenation is excluded, since the double-sided graphane-embedded structure is energetically more favorable. The 1D C4H nanotubes, rolled up by the C4H layer, exhibit excellent thermodynamic properties and all have a wide band gap regardless of the tube diameter and chirality. In contrast, cutting the C4H layer into 1D C4H nanoribbons can result in rich electronic characteristics: they can be metallic or semiconducting depending on the chirality and edge configuration.</abstract><cop>Columbus, OH</cop><pub>American Chemical Society</pub><doi>10.1021/jp212499h</doi><tpages>9</tpages></addata></record> |
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source | American Chemical Society:Jisc Collections:American Chemical Society Read & Publish Agreement 2022-2024 (Reading list) |
subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Cross-disciplinary physics: materials science rheology Electron states Electron states and collective excitations in thin films, multilayers, quantum wells, mesoscopic and nanoscale systems Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures Exact sciences and technology Fullerenes and related materials diamonds, graphite Materials science Methods of electronic structure calculations Nanoscale materials and structures: fabrication and characterization Nanotubes Physics Specific materials |
title | Patterned Partially Hydrogenated Graphene (C4H) and Its One-Dimensional Analogues: A Computational Study |
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