Magnetic Susceptibility of Molecular Carbon: Nanotubes and Fullerite
Elemental carbon can be synthesized in a variety of geometrical forms, from three-dimensional extended structures (diamond) to finite molecules (C$_{60}$ fullerite). Results are presented here on the magnetic susceptibility of the least well-understood members of this family, nanotubes and C$_{60}$...
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Veröffentlicht in: | Science (American Association for the Advancement of Science) 1994-07, Vol.265 (5168), p.84-86 |
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creator | Ramirez, A. P. Haddon, R. C. Zhou, O. Fleming, R. M. Zhang, J. McClure, S. M. Smalley, R. E. |
description | Elemental carbon can be synthesized in a variety of geometrical forms, from three-dimensional extended structures (diamond) to finite molecules (C$_{60}$ fullerite). Results are presented here on the magnetic susceptibility of the least well-understood members of this family, nanotubes and C$_{60}$ fullerite. (i) Nanotubes represent the cylindrical form of carbon, intermediate between graphite and fullerite. They are found to have significantly larger orientation-averaged susceptibility, on a per carbon basis, than any other form of elemental carbon. This susceptibility implies an average band structure among nanotubes similar to that of graphite. (ii) High-resolution magnetic susceptibility data on C$_{60}$ fullerite near the molecular orientational-ordering transition at 259 K show a sharp jump corresponding to 2.5 centimeter-gram-second parts per million per mole of C$_{60}$. This jump directly demonstrates the effect of an intermolecular cooperative transition on an intramolecular electronic property, where the susceptibility jump may be ascribed to a change in the shape of the molecule due to lattice forces. |
doi_str_mv | 10.1126/science.265.5168.84 |
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P. ; Haddon, R. C. ; Zhou, O. ; Fleming, R. M. ; Zhang, J. ; McClure, S. M. ; Smalley, R. E.</creator><creatorcontrib>Ramirez, A. P. ; Haddon, R. C. ; Zhou, O. ; Fleming, R. M. ; Zhang, J. ; McClure, S. M. ; Smalley, R. E.</creatorcontrib><description>Elemental carbon can be synthesized in a variety of geometrical forms, from three-dimensional extended structures (diamond) to finite molecules (C$_{60}$ fullerite). Results are presented here on the magnetic susceptibility of the least well-understood members of this family, nanotubes and C$_{60}$ fullerite. (i) Nanotubes represent the cylindrical form of carbon, intermediate between graphite and fullerite. They are found to have significantly larger orientation-averaged susceptibility, on a per carbon basis, than any other form of elemental carbon. This susceptibility implies an average band structure among nanotubes similar to that of graphite. (ii) High-resolution magnetic susceptibility data on C$_{60}$ fullerite near the molecular orientational-ordering transition at 259 K show a sharp jump corresponding to 2.5 centimeter-gram-second parts per million per mole of C$_{60}$. This jump directly demonstrates the effect of an intermolecular cooperative transition on an intramolecular electronic property, where the susceptibility jump may be ascribed to a change in the shape of the molecule due to lattice forces.</description><identifier>ISSN: 0036-8075</identifier><identifier>EISSN: 1095-9203</identifier><identifier>DOI: 10.1126/science.265.5168.84</identifier><identifier>PMID: 17774693</identifier><identifier>CODEN: SCIEAS</identifier><language>eng</language><publisher>Washington, DC: American Society for the Advancement of Science</publisher><subject>Carbon ; Carbon nanotubes ; Chemical bonding ; Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Electronic structure ; Exact sciences and technology ; Graphite ; Magnetic permeability ; Magnetic properties and materials ; Magnetic susceptibility ; Magnetically ordered materials: other intrinsic properties ; Molecular structure ; Molecules ; Nanotubes ; Physics ; Ring currents ; Saturation moments and magnetic susceptibilities</subject><ispartof>Science (American Association for the Advancement of Science), 1994-07, Vol.265 (5168), p.84-86</ispartof><rights>Copyright 1994 American Association for the Advancement of Science</rights><rights>1994 INIST-CNRS</rights><rights>COPYRIGHT 1994 American Association for the Advancement of Science</rights><rights>COPYRIGHT 1994 American Association for the Advancement of Science</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c722t-a936eb468c1423d00f1ef40d5a768cf8672dc77a2e533bb6f16f16dd89f6e8193</citedby><cites>FETCH-LOGICAL-c722t-a936eb468c1423d00f1ef40d5a768cf8672dc77a2e533bb6f16f16dd89f6e8193</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.jstor.org/stable/pdf/2884365$$EPDF$$P50$$Gjstor$$H</linktopdf><linktohtml>$$Uhttps://www.jstor.org/stable/2884365$$EHTML$$P50$$Gjstor$$H</linktohtml><link.rule.ids>314,776,780,799,2871,2872,27901,27902,57992,58225</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=4127272$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/17774693$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Ramirez, A. P.</creatorcontrib><creatorcontrib>Haddon, R. C.</creatorcontrib><creatorcontrib>Zhou, O.</creatorcontrib><creatorcontrib>Fleming, R. M.</creatorcontrib><creatorcontrib>Zhang, J.</creatorcontrib><creatorcontrib>McClure, S. M.</creatorcontrib><creatorcontrib>Smalley, R. E.</creatorcontrib><title>Magnetic Susceptibility of Molecular Carbon: Nanotubes and Fullerite</title><title>Science (American Association for the Advancement of Science)</title><addtitle>Science</addtitle><description>Elemental carbon can be synthesized in a variety of geometrical forms, from three-dimensional extended structures (diamond) to finite molecules (C$_{60}$ fullerite). Results are presented here on the magnetic susceptibility of the least well-understood members of this family, nanotubes and C$_{60}$ fullerite. (i) Nanotubes represent the cylindrical form of carbon, intermediate between graphite and fullerite. They are found to have significantly larger orientation-averaged susceptibility, on a per carbon basis, than any other form of elemental carbon. This susceptibility implies an average band structure among nanotubes similar to that of graphite. (ii) High-resolution magnetic susceptibility data on C$_{60}$ fullerite near the molecular orientational-ordering transition at 259 K show a sharp jump corresponding to 2.5 centimeter-gram-second parts per million per mole of C$_{60}$. This jump directly demonstrates the effect of an intermolecular cooperative transition on an intramolecular electronic property, where the susceptibility jump may be ascribed to a change in the shape of the molecule due to lattice forces.</description><subject>Carbon</subject><subject>Carbon nanotubes</subject><subject>Chemical bonding</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Electronic structure</subject><subject>Exact sciences and technology</subject><subject>Graphite</subject><subject>Magnetic permeability</subject><subject>Magnetic properties and materials</subject><subject>Magnetic susceptibility</subject><subject>Magnetically ordered materials: other intrinsic properties</subject><subject>Molecular structure</subject><subject>Molecules</subject><subject>Nanotubes</subject><subject>Physics</subject><subject>Ring currents</subject><subject>Saturation moments and magnetic susceptibilities</subject><issn>0036-8075</issn><issn>1095-9203</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1994</creationdate><recordtype>article</recordtype><recordid>eNqN0luLEzEUAOBBFLeu_gJF5kHUh52ay-Qyvq3VrQvd7cOqr0Mmc1KypJOaZMD996a0rBSKlAQCOd9JQs4pitcYTTEm_FPUFgYNU8LZlGEup7J-UkwwaljVEESfFhOEKK8kEuyseBHjPUI51tDnxRkWQtS8oZPi641aDZCsLu_GqGGTbGedTQ-lN-WNd6BHp0I5U6Hzw-fyVg0-jR3EUg19eTU6B8EmeFk8M8pFeLVfz4ufV99-zL5Xi-X8ena5qLQgJFWqoRy6mkuNa0J7hAwGU6OeKZH3jOSC9FoIRYBR2nXc4O3se9kYDhI39Lz4sDt3E_zvEWJq1zY_2jk1gB9jKygliDS1yPL9fyXhdS1JvT3yYgdXykFrB-NTUHoFAwTl_ADG5u1LzJhkpOGZV0d4Hj2srT7mPx74TBL8SSs1xthe392eTJe_TqZf5qdSOV8c0ItjVPtc5RW0uZKz5QGnO66DjzGAaTfBrlV4aDFqtw3a7hs0fzZrtw3ayjpnvd0XZuzW0P_L2XdkBu_2QEWtnAlq0DY-uhoTkUdmb3bsPiYfHsNE5js4o38BwxTzwA</recordid><startdate>19940701</startdate><enddate>19940701</enddate><creator>Ramirez, A. P.</creator><creator>Haddon, R. C.</creator><creator>Zhou, O.</creator><creator>Fleming, R. M.</creator><creator>Zhang, J.</creator><creator>McClure, S. M.</creator><creator>Smalley, R. E.</creator><general>American Society for the Advancement of Science</general><general>American Association for the Advancement of Science</general><scope>IQODW</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8GL</scope><scope>IBG</scope><scope>IOV</scope><scope>ISN</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope></search><sort><creationdate>19940701</creationdate><title>Magnetic Susceptibility of Molecular Carbon: Nanotubes and Fullerite</title><author>Ramirez, A. P. ; Haddon, R. C. ; Zhou, O. ; Fleming, R. M. ; Zhang, J. ; McClure, S. M. ; Smalley, R. E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c722t-a936eb468c1423d00f1ef40d5a768cf8672dc77a2e533bb6f16f16dd89f6e8193</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1994</creationdate><topic>Carbon</topic><topic>Carbon nanotubes</topic><topic>Chemical bonding</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Electronic structure</topic><topic>Exact sciences and technology</topic><topic>Graphite</topic><topic>Magnetic permeability</topic><topic>Magnetic properties and materials</topic><topic>Magnetic susceptibility</topic><topic>Magnetically ordered materials: other intrinsic properties</topic><topic>Molecular structure</topic><topic>Molecules</topic><topic>Nanotubes</topic><topic>Physics</topic><topic>Ring currents</topic><topic>Saturation moments and magnetic susceptibilities</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ramirez, A. P.</creatorcontrib><creatorcontrib>Haddon, R. C.</creatorcontrib><creatorcontrib>Zhou, O.</creatorcontrib><creatorcontrib>Fleming, R. M.</creatorcontrib><creatorcontrib>Zhang, J.</creatorcontrib><creatorcontrib>McClure, S. M.</creatorcontrib><creatorcontrib>Smalley, R. 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E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Magnetic Susceptibility of Molecular Carbon: Nanotubes and Fullerite</atitle><jtitle>Science (American Association for the Advancement of Science)</jtitle><addtitle>Science</addtitle><date>1994-07-01</date><risdate>1994</risdate><volume>265</volume><issue>5168</issue><spage>84</spage><epage>86</epage><pages>84-86</pages><issn>0036-8075</issn><eissn>1095-9203</eissn><coden>SCIEAS</coden><abstract>Elemental carbon can be synthesized in a variety of geometrical forms, from three-dimensional extended structures (diamond) to finite molecules (C$_{60}$ fullerite). Results are presented here on the magnetic susceptibility of the least well-understood members of this family, nanotubes and C$_{60}$ fullerite. (i) Nanotubes represent the cylindrical form of carbon, intermediate between graphite and fullerite. They are found to have significantly larger orientation-averaged susceptibility, on a per carbon basis, than any other form of elemental carbon. This susceptibility implies an average band structure among nanotubes similar to that of graphite. (ii) High-resolution magnetic susceptibility data on C$_{60}$ fullerite near the molecular orientational-ordering transition at 259 K show a sharp jump corresponding to 2.5 centimeter-gram-second parts per million per mole of C$_{60}$. This jump directly demonstrates the effect of an intermolecular cooperative transition on an intramolecular electronic property, where the susceptibility jump may be ascribed to a change in the shape of the molecule due to lattice forces.</abstract><cop>Washington, DC</cop><pub>American Society for the Advancement of Science</pub><pmid>17774693</pmid><doi>10.1126/science.265.5168.84</doi><tpages>3</tpages></addata></record> |
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subjects | Carbon Carbon nanotubes Chemical bonding Condensed matter: electronic structure, electrical, magnetic, and optical properties Electronic structure Exact sciences and technology Graphite Magnetic permeability Magnetic properties and materials Magnetic susceptibility Magnetically ordered materials: other intrinsic properties Molecular structure Molecules Nanotubes Physics Ring currents Saturation moments and magnetic susceptibilities |
title | Magnetic Susceptibility of Molecular Carbon: Nanotubes and Fullerite |
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