Molecular dynamics simulation of C60 encapsulated in boron nitride nanotubes
We investigate the C60 chain encapsulated in boron nitride (BN) nanotubes using molecular‐dynamics simulation. The most favorable BN nanotubes for encapsulation of C60 molecules are (10, 10) and (17, 0) with energy gains of 3.83 and 3.61 eV per C60 for (n, n) and (n, 0) BN nanotubes, respectively. F...
Gespeichert in:
Veröffentlicht in: | Physica status solidi. B. Basic research 2004-07, Vol.241 (8), p.1783-1788 |
---|---|
Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 1788 |
---|---|
container_issue | 8 |
container_start_page | 1783 |
container_title | Physica status solidi. B. Basic research |
container_volume | 241 |
creator | Moon, Won Ha Son, Myung Sik Lee, Jun Ha Hwang, Ho Jung |
description | We investigate the C60 chain encapsulated in boron nitride (BN) nanotubes using molecular‐dynamics simulation. The most favorable BN nanotubes for encapsulation of C60 molecules are (10, 10) and (17, 0) with energy gains of 3.83 and 3.61 eV per C60 for (n, n) and (n, 0) BN nanotubes, respectively. For the diffusion of a C60 into the tube, the position of atoms of a C60 must be not located above the outer wall of the BN nanotube. The C60 located above the outer wall is quickly absorbed and moves on the surface of the tube. The C60 absorbed on the surface is not spontaneously encapsulated inside the tube, which is due to the energy barrier (0.48 eV) of the edge of the BN nanotube. We also calculate the energy barrier for drawing C60 outside the (10, 10) BN nanotube, which is above 3.92 eV. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) |
doi_str_mv | 10.1002/pssb.200402032 |
format | Article |
fullrecord | <record><control><sourceid>wiley_pasca</sourceid><recordid>TN_cdi_pascalfrancis_primary_15945381</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>PSSB200402032</sourcerecordid><originalsourceid>FETCH-LOGICAL-i1862-69bd916e709de23cf5f3cb7c56079b85b206597aaa6c0077e992f93a740b218d3</originalsourceid><addsrcrecordid>eNpFkD1PwzAQhi0EEqWwMnthTDnbsR2PEEGBli8VxGjZjiMZUqeKU0H_PamKynS69-N0ehA6JzAhAPRylZKdUIAcKDB6gEaEU5IxxckhGgGTkBEl6TE6SekTACRhZITmj23j3boxHa420SyDSziF5SD0oY24rXEpAPvozCptRV_hELFtu8GMoe9C5XE0se3X1qdTdFSbJvmzvzlG77c3b-VdNn-e3pdX8yyQQtBMKFspIrwEVXnKXM1r5qx0XIBUtuCWguBKGmOEG_6UXilaK2ZkDpaSomJjdLG7uzLJmabuTHQh6VUXlqbbaMJVzllBhpza5b5D4zf_PugtML0FpvfA9Mticb3fhm6264bU-59913RfWkgmuf54mupimj-UsxnVr-wXrJlwag</addsrcrecordid><sourcetype>Index Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Molecular dynamics simulation of C60 encapsulated in boron nitride nanotubes</title><source>Access via Wiley Online Library</source><creator>Moon, Won Ha ; Son, Myung Sik ; Lee, Jun Ha ; Hwang, Ho Jung</creator><creatorcontrib>Moon, Won Ha ; Son, Myung Sik ; Lee, Jun Ha ; Hwang, Ho Jung</creatorcontrib><description>We investigate the C60 chain encapsulated in boron nitride (BN) nanotubes using molecular‐dynamics simulation. The most favorable BN nanotubes for encapsulation of C60 molecules are (10, 10) and (17, 0) with energy gains of 3.83 and 3.61 eV per C60 for (n, n) and (n, 0) BN nanotubes, respectively. For the diffusion of a C60 into the tube, the position of atoms of a C60 must be not located above the outer wall of the BN nanotube. The C60 located above the outer wall is quickly absorbed and moves on the surface of the tube. The C60 absorbed on the surface is not spontaneously encapsulated inside the tube, which is due to the energy barrier (0.48 eV) of the edge of the BN nanotube. We also calculate the energy barrier for drawing C60 outside the (10, 10) BN nanotube, which is above 3.92 eV. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)</description><identifier>ISSN: 0370-1972</identifier><identifier>EISSN: 1521-3951</identifier><identifier>DOI: 10.1002/pssb.200402032</identifier><identifier>CODEN: PSSBBD</identifier><language>eng</language><publisher>Berlin: WILEY-VCH Verlag</publisher><subject>31.15.Qg ; 61.46.+w ; 61.48.+c ; 71.15.Pd ; 71.20.Tx ; Cross-disciplinary physics: materials science; rheology ; Exact sciences and technology ; Materials science ; Nanoscale materials and structures: fabrication and characterization ; Nanotubes ; Physics</subject><ispartof>Physica status solidi. B. Basic research, 2004-07, Vol.241 (8), p.1783-1788</ispartof><rights>Copyright © 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim</rights><rights>2004 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fpssb.200402032$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fpssb.200402032$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,27924,27925,45574,45575</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=15945381$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Moon, Won Ha</creatorcontrib><creatorcontrib>Son, Myung Sik</creatorcontrib><creatorcontrib>Lee, Jun Ha</creatorcontrib><creatorcontrib>Hwang, Ho Jung</creatorcontrib><title>Molecular dynamics simulation of C60 encapsulated in boron nitride nanotubes</title><title>Physica status solidi. B. Basic research</title><addtitle>phys. stat. sol. (b)</addtitle><description>We investigate the C60 chain encapsulated in boron nitride (BN) nanotubes using molecular‐dynamics simulation. The most favorable BN nanotubes for encapsulation of C60 molecules are (10, 10) and (17, 0) with energy gains of 3.83 and 3.61 eV per C60 for (n, n) and (n, 0) BN nanotubes, respectively. For the diffusion of a C60 into the tube, the position of atoms of a C60 must be not located above the outer wall of the BN nanotube. The C60 located above the outer wall is quickly absorbed and moves on the surface of the tube. The C60 absorbed on the surface is not spontaneously encapsulated inside the tube, which is due to the energy barrier (0.48 eV) of the edge of the BN nanotube. We also calculate the energy barrier for drawing C60 outside the (10, 10) BN nanotube, which is above 3.92 eV. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)</description><subject>31.15.Qg</subject><subject>61.46.+w</subject><subject>61.48.+c</subject><subject>71.15.Pd</subject><subject>71.20.Tx</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Exact sciences and technology</subject><subject>Materials science</subject><subject>Nanoscale materials and structures: fabrication and characterization</subject><subject>Nanotubes</subject><subject>Physics</subject><issn>0370-1972</issn><issn>1521-3951</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><recordid>eNpFkD1PwzAQhi0EEqWwMnthTDnbsR2PEEGBli8VxGjZjiMZUqeKU0H_PamKynS69-N0ehA6JzAhAPRylZKdUIAcKDB6gEaEU5IxxckhGgGTkBEl6TE6SekTACRhZITmj23j3boxHa420SyDSziF5SD0oY24rXEpAPvozCptRV_hELFtu8GMoe9C5XE0se3X1qdTdFSbJvmzvzlG77c3b-VdNn-e3pdX8yyQQtBMKFspIrwEVXnKXM1r5qx0XIBUtuCWguBKGmOEG_6UXilaK2ZkDpaSomJjdLG7uzLJmabuTHQh6VUXlqbbaMJVzllBhpza5b5D4zf_PugtML0FpvfA9Mticb3fhm6264bU-59913RfWkgmuf54mupimj-UsxnVr-wXrJlwag</recordid><startdate>200407</startdate><enddate>200407</enddate><creator>Moon, Won Ha</creator><creator>Son, Myung Sik</creator><creator>Lee, Jun Ha</creator><creator>Hwang, Ho Jung</creator><general>WILEY-VCH Verlag</general><general>WILEY‐VCH Verlag</general><general>Wiley</general><scope>BSCLL</scope><scope>IQODW</scope></search><sort><creationdate>200407</creationdate><title>Molecular dynamics simulation of C60 encapsulated in boron nitride nanotubes</title><author>Moon, Won Ha ; Son, Myung Sik ; Lee, Jun Ha ; Hwang, Ho Jung</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i1862-69bd916e709de23cf5f3cb7c56079b85b206597aaa6c0077e992f93a740b218d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2004</creationdate><topic>31.15.Qg</topic><topic>61.46.+w</topic><topic>61.48.+c</topic><topic>71.15.Pd</topic><topic>71.20.Tx</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Exact sciences and technology</topic><topic>Materials science</topic><topic>Nanoscale materials and structures: fabrication and characterization</topic><topic>Nanotubes</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Moon, Won Ha</creatorcontrib><creatorcontrib>Son, Myung Sik</creatorcontrib><creatorcontrib>Lee, Jun Ha</creatorcontrib><creatorcontrib>Hwang, Ho Jung</creatorcontrib><collection>Istex</collection><collection>Pascal-Francis</collection><jtitle>Physica status solidi. B. Basic research</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Moon, Won Ha</au><au>Son, Myung Sik</au><au>Lee, Jun Ha</au><au>Hwang, Ho Jung</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Molecular dynamics simulation of C60 encapsulated in boron nitride nanotubes</atitle><jtitle>Physica status solidi. B. Basic research</jtitle><addtitle>phys. stat. sol. (b)</addtitle><date>2004-07</date><risdate>2004</risdate><volume>241</volume><issue>8</issue><spage>1783</spage><epage>1788</epage><pages>1783-1788</pages><issn>0370-1972</issn><eissn>1521-3951</eissn><coden>PSSBBD</coden><abstract>We investigate the C60 chain encapsulated in boron nitride (BN) nanotubes using molecular‐dynamics simulation. The most favorable BN nanotubes for encapsulation of C60 molecules are (10, 10) and (17, 0) with energy gains of 3.83 and 3.61 eV per C60 for (n, n) and (n, 0) BN nanotubes, respectively. For the diffusion of a C60 into the tube, the position of atoms of a C60 must be not located above the outer wall of the BN nanotube. The C60 located above the outer wall is quickly absorbed and moves on the surface of the tube. The C60 absorbed on the surface is not spontaneously encapsulated inside the tube, which is due to the energy barrier (0.48 eV) of the edge of the BN nanotube. We also calculate the energy barrier for drawing C60 outside the (10, 10) BN nanotube, which is above 3.92 eV. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)</abstract><cop>Berlin</cop><pub>WILEY-VCH Verlag</pub><doi>10.1002/pssb.200402032</doi><tpages>6</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0370-1972 |
ispartof | Physica status solidi. B. Basic research, 2004-07, Vol.241 (8), p.1783-1788 |
issn | 0370-1972 1521-3951 |
language | eng |
recordid | cdi_pascalfrancis_primary_15945381 |
source | Access via Wiley Online Library |
subjects | 31.15.Qg 61.46.+w 61.48.+c 71.15.Pd 71.20.Tx Cross-disciplinary physics: materials science rheology Exact sciences and technology Materials science Nanoscale materials and structures: fabrication and characterization Nanotubes Physics |
title | Molecular dynamics simulation of C60 encapsulated in boron nitride nanotubes |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-26T17%3A47%3A54IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-wiley_pasca&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Molecular%20dynamics%20simulation%20of%20C60%20encapsulated%20in%20boron%20nitride%20nanotubes&rft.jtitle=Physica%20status%20solidi.%20B.%20Basic%20research&rft.au=Moon,%20Won%20Ha&rft.date=2004-07&rft.volume=241&rft.issue=8&rft.spage=1783&rft.epage=1788&rft.pages=1783-1788&rft.issn=0370-1972&rft.eissn=1521-3951&rft.coden=PSSBBD&rft_id=info:doi/10.1002/pssb.200402032&rft_dat=%3Cwiley_pasca%3EPSSB200402032%3C/wiley_pasca%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true |