Single Jump Mechanisms for Large Cluster Diffusion on Metal Surfaces
The random motion of large, two-dimensional adatom clusters and vacancy clusters over a metal surface is described by a diffusion coefficient {ital D}{proportional_to}{ital d}{sup {minus}{ital n}}, where {ital d} is the diameter of the cluster and the integer {ital n} identifies the diffusion mechan...
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Veröffentlicht in: | Physical Review Letters 1995-08, Vol.75 (8), p.1574-1577 |
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description | The random motion of large, two-dimensional adatom clusters and vacancy clusters over a metal surface is described by a diffusion coefficient {ital D}{proportional_to}{ital d}{sup {minus}{ital n}}, where {ital d} is the diameter of the cluster and the integer {ital n} identifies the diffusion mechanism. For {ital circular} clusters, {ital n}=3 when center-of-mass motion occurs by adatom diffusion along the periphery of the cluster, while {ital n}=2 or 1 when cluster diffusion occurs by {ital correlated} or {ital uncorrelated} adatom evaporation and condensation, respectively. A {ital faceted} adatom cluster diffuses by evaporation and condensation of facet ledges, giving {ital n}=0 when cluster diffusion is determined by the rate at which erosion of a ledge is initiated. |
doi_str_mv | 10.1103/physrevlett.75.1574 |
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For {ital circular} clusters, {ital n}=3 when center-of-mass motion occurs by adatom diffusion along the periphery of the cluster, while {ital n}=2 or 1 when cluster diffusion occurs by {ital correlated} or {ital uncorrelated} adatom evaporation and condensation, respectively. A {ital faceted} adatom cluster diffuses by evaporation and condensation of facet ledges, giving {ital n}=0 when cluster diffusion is determined by the rate at which erosion of a ledge is initiated.</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><identifier>DOI: 10.1103/physrevlett.75.1574</identifier><identifier>PMID: 10060332</identifier><language>eng</language><publisher>United States</publisher><subject>ADSORPTION ; ATOMIC CLUSTERS ; DIFFUSION ; MATERIALS SCIENCE ; METALS ; MORPHOLOGY ; SURFACE PROPERTIES ; VACANCIES</subject><ispartof>Physical Review Letters, 1995-08, Vol.75 (8), p.1574-1577</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c395t-549d626f214482abf07726d02dcd4b070b1f7b71b9a9b3d8293d7d90fa61ff2d3</citedby><cites>FETCH-LOGICAL-c395t-549d626f214482abf07726d02dcd4b070b1f7b71b9a9b3d8293d7d90fa61ff2d3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,881,2862,2863,27903,27904</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/10060332$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/116009$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Van Siclen, Clinton DeW</creatorcontrib><creatorcontrib>Idaho National Engineering Lab</creatorcontrib><title>Single Jump Mechanisms for Large Cluster Diffusion on Metal Surfaces</title><title>Physical Review Letters</title><addtitle>Phys Rev Lett</addtitle><description>The random motion of large, two-dimensional adatom clusters and vacancy clusters over a metal surface is described by a diffusion coefficient {ital D}{proportional_to}{ital d}{sup {minus}{ital n}}, where {ital d} is the diameter of the cluster and the integer {ital n} identifies the diffusion mechanism. For {ital circular} clusters, {ital n}=3 when center-of-mass motion occurs by adatom diffusion along the periphery of the cluster, while {ital n}=2 or 1 when cluster diffusion occurs by {ital correlated} or {ital uncorrelated} adatom evaporation and condensation, respectively. A {ital faceted} adatom cluster diffuses by evaporation and condensation of facet ledges, giving {ital n}=0 when cluster diffusion is determined by the rate at which erosion of a ledge is initiated.</description><subject>ADSORPTION</subject><subject>ATOMIC CLUSTERS</subject><subject>DIFFUSION</subject><subject>MATERIALS SCIENCE</subject><subject>METALS</subject><subject>MORPHOLOGY</subject><subject>SURFACE PROPERTIES</subject><subject>VACANCIES</subject><issn>0031-9007</issn><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1995</creationdate><recordtype>article</recordtype><recordid>eNpNkMlKBDEQhoMoOi5PIEh789JjVdLd6RxlxpURxeUc0lm0pZcxSQu-vZHxIBTU5fv_Kj5CjhHmiMDO1-_fwduvzsY45-UcS15skRkCFzlHLLbJDIBhLgD4HtkP4QMAkFb1LtlDgAoYozOyfG6Ht85md1O_zu6tfldDG_qQudFnK-XfbLbophCtz5atc1NoxyFLc2-j6rLnyTulbTgkO051wR797QPyenX5srjJVw_Xt4uLVa6ZKGNeFsJUtHIUi6KmqnHAOa0MUKNN0QCHBh1vODZCiYaZmgpmuBHgVIXOUcMOyOmmdwyxlUG3MT2sx2GwOkrECkAk5mzDrP34OdkQZd8GbbtODXacgsS6FDSRNSaUbVDtx5BUOrn2ba_8t0SQv4rlY1L8ZL9WSbHkpfxVnFInfwemprfmX2bjlP0AwTV5WQ</recordid><startdate>19950821</startdate><enddate>19950821</enddate><creator>Van Siclen, Clinton DeW</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>OTOTI</scope></search><sort><creationdate>19950821</creationdate><title>Single Jump Mechanisms for Large Cluster Diffusion on Metal Surfaces</title><author>Van Siclen, Clinton DeW</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c395t-549d626f214482abf07726d02dcd4b070b1f7b71b9a9b3d8293d7d90fa61ff2d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1995</creationdate><topic>ADSORPTION</topic><topic>ATOMIC CLUSTERS</topic><topic>DIFFUSION</topic><topic>MATERIALS SCIENCE</topic><topic>METALS</topic><topic>MORPHOLOGY</topic><topic>SURFACE PROPERTIES</topic><topic>VACANCIES</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Van Siclen, Clinton DeW</creatorcontrib><creatorcontrib>Idaho National Engineering Lab</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Physical Review Letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Van Siclen, Clinton DeW</au><aucorp>Idaho National Engineering Lab</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Single Jump Mechanisms for Large Cluster Diffusion on Metal Surfaces</atitle><jtitle>Physical Review Letters</jtitle><addtitle>Phys Rev Lett</addtitle><date>1995-08-21</date><risdate>1995</risdate><volume>75</volume><issue>8</issue><spage>1574</spage><epage>1577</epage><pages>1574-1577</pages><issn>0031-9007</issn><eissn>1079-7114</eissn><abstract>The random motion of large, two-dimensional adatom clusters and vacancy clusters over a metal surface is described by a diffusion coefficient {ital D}{proportional_to}{ital d}{sup {minus}{ital n}}, where {ital d} is the diameter of the cluster and the integer {ital n} identifies the diffusion mechanism. For {ital circular} clusters, {ital n}=3 when center-of-mass motion occurs by adatom diffusion along the periphery of the cluster, while {ital n}=2 or 1 when cluster diffusion occurs by {ital correlated} or {ital uncorrelated} adatom evaporation and condensation, respectively. A {ital faceted} adatom cluster diffuses by evaporation and condensation of facet ledges, giving {ital n}=0 when cluster diffusion is determined by the rate at which erosion of a ledge is initiated.</abstract><cop>United States</cop><pmid>10060332</pmid><doi>10.1103/physrevlett.75.1574</doi><tpages>4</tpages></addata></record> |
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subjects | ADSORPTION ATOMIC CLUSTERS DIFFUSION MATERIALS SCIENCE METALS MORPHOLOGY SURFACE PROPERTIES VACANCIES |
title | Single Jump Mechanisms for Large Cluster Diffusion on Metal Surfaces |
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