Monte Carlo simulation of equilibrium L1 ordering in FePt nanoparticles
First, second, and third nearest-neighbor mixing potentials for FePt alloys were calculated from first principles using the Connolly–Williams approach. Using the mixing potentials obtained in this manner, the dependency of equilibrium L10 ordering on temperature was studied for bulk and for a spheri...
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description | First, second, and third nearest-neighbor mixing potentials for FePt alloys were calculated from first principles using the Connolly–Williams approach. Using the mixing potentials obtained in this manner, the dependency of equilibrium L10 ordering on temperature was studied for bulk and for a spherical nanoparticle with a 3.5-nm diameter at equiatomic composition by use of Monte Carlo simulation and the analytical ring approximation. The calculated order-disorder temperature for bulk (1495–1514K) was in relatively good agreement (4% error) with the experimental value (1572K). For nanoparticles of finite size, the (long-range) order parameter changed continuously from unity to zero with increasing temperature. Rather than a discontinuity indicative of a phase-transition we obtained an inflection point in the order as a function of temperature. This inflection point occurred at a temperature below the bulk phase-transition temperature and which decreased as the particle size decreased. Our calculations predict that 3.5-nm diameter particles in configurational equilibrium at 600°C (a typical annealing temperature for promoting L10 ordering) have an L10 order parameter of 0.83 (compared to a maximum possible value equal to unity). According to our investigations, the experimental absence of a (relatively) high L10 order in 3.5-nm diameter nanoparticles annealed at 600°C or below is primarily a problem of kinetics rather than equilibrium. |
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V. ; Velev, J. ; Butler, W. H.</creator><creatorcontrib>Chepulskii, R. V. ; Velev, J. ; Butler, W. H.</creatorcontrib><description>First, second, and third nearest-neighbor mixing potentials for FePt alloys were calculated from first principles using the Connolly–Williams approach. Using the mixing potentials obtained in this manner, the dependency of equilibrium L10 ordering on temperature was studied for bulk and for a spherical nanoparticle with a 3.5-nm diameter at equiatomic composition by use of Monte Carlo simulation and the analytical ring approximation. The calculated order-disorder temperature for bulk (1495–1514K) was in relatively good agreement (4% error) with the experimental value (1572K). For nanoparticles of finite size, the (long-range) order parameter changed continuously from unity to zero with increasing temperature. Rather than a discontinuity indicative of a phase-transition we obtained an inflection point in the order as a function of temperature. This inflection point occurred at a temperature below the bulk phase-transition temperature and which decreased as the particle size decreased. Our calculations predict that 3.5-nm diameter particles in configurational equilibrium at 600°C (a typical annealing temperature for promoting L10 ordering) have an L10 order parameter of 0.83 (compared to a maximum possible value equal to unity). According to our investigations, the experimental absence of a (relatively) high L10 order in 3.5-nm diameter nanoparticles annealed at 600°C or below is primarily a problem of kinetics rather than equilibrium.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.1852351</identifier><language>eng</language><publisher>United States</publisher><subject>ANNEALING ; BINARY ALLOY SYSTEMS ; COMPUTERIZED SIMULATION ; FERROMAGNETIC MATERIALS ; IRON ALLOYS ; MATERIALS SCIENCE ; MIXING ; MONTE CARLO METHOD ; ORDER PARAMETERS ; ORDER-DISORDER TRANSFORMATIONS ; PLATINUM ALLOYS ; POTENTIALS ; TEMPERATURE DEPENDENCE ; TEMPERATURE RANGE 0400-1000 K ; TEMPERATURE RANGE 1000-4000 K ; TRANSITION TEMPERATURE</subject><ispartof>Journal of applied physics, 2005-05, Vol.97 (10)</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c253t-e3b6bc14c90251f7c58200545dbc1c8e8b80e34988927e4686c181e9aa31ed8c3</citedby><cites>FETCH-LOGICAL-c253t-e3b6bc14c90251f7c58200545dbc1c8e8b80e34988927e4686c181e9aa31ed8c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,315,781,785,886,27929,27930</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/20711646$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Chepulskii, R. V.</creatorcontrib><creatorcontrib>Velev, J.</creatorcontrib><creatorcontrib>Butler, W. H.</creatorcontrib><title>Monte Carlo simulation of equilibrium L1 ordering in FePt nanoparticles</title><title>Journal of applied physics</title><description>First, second, and third nearest-neighbor mixing potentials for FePt alloys were calculated from first principles using the Connolly–Williams approach. Using the mixing potentials obtained in this manner, the dependency of equilibrium L10 ordering on temperature was studied for bulk and for a spherical nanoparticle with a 3.5-nm diameter at equiatomic composition by use of Monte Carlo simulation and the analytical ring approximation. The calculated order-disorder temperature for bulk (1495–1514K) was in relatively good agreement (4% error) with the experimental value (1572K). For nanoparticles of finite size, the (long-range) order parameter changed continuously from unity to zero with increasing temperature. Rather than a discontinuity indicative of a phase-transition we obtained an inflection point in the order as a function of temperature. This inflection point occurred at a temperature below the bulk phase-transition temperature and which decreased as the particle size decreased. Our calculations predict that 3.5-nm diameter particles in configurational equilibrium at 600°C (a typical annealing temperature for promoting L10 ordering) have an L10 order parameter of 0.83 (compared to a maximum possible value equal to unity). According to our investigations, the experimental absence of a (relatively) high L10 order in 3.5-nm diameter nanoparticles annealed at 600°C or below is primarily a problem of kinetics rather than equilibrium.</description><subject>ANNEALING</subject><subject>BINARY ALLOY SYSTEMS</subject><subject>COMPUTERIZED SIMULATION</subject><subject>FERROMAGNETIC MATERIALS</subject><subject>IRON ALLOYS</subject><subject>MATERIALS SCIENCE</subject><subject>MIXING</subject><subject>MONTE CARLO METHOD</subject><subject>ORDER PARAMETERS</subject><subject>ORDER-DISORDER TRANSFORMATIONS</subject><subject>PLATINUM ALLOYS</subject><subject>POTENTIALS</subject><subject>TEMPERATURE DEPENDENCE</subject><subject>TEMPERATURE RANGE 0400-1000 K</subject><subject>TEMPERATURE RANGE 1000-4000 K</subject><subject>TRANSITION TEMPERATURE</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNotkMFKAzEURYMoWKsL_yDgysXU9yaTmWQpxVahogtdh0z6RiPTpCbpwr-3pV1duBzO4jB2izBDaMUDzlDJWkg8YxMEpatOSjhnE4AaK6U7fcmucv4BQFRCT9jyNYZCfG7TGHn2m91oi4-Bx4HT786Pvk9-t-Er5DGtKfnwxX3gC3ovPNgQtzYV70bK1-xisGOmm9NO2efi6WP-XK3eli_zx1XlailKRaJve4eN01BLHDonVQ0gG7nev06R6hWQaLRSuu6oaVXrUCFpawXSWjkxZXdHb8zFm-x8IfftYgjkiqmhQ2ybdk_dHymXYs6JBrNNfmPTn0Ewh04GzamT-AerC1jY</recordid><startdate>20050515</startdate><enddate>20050515</enddate><creator>Chepulskii, R. 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H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c253t-e3b6bc14c90251f7c58200545dbc1c8e8b80e34988927e4686c181e9aa31ed8c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><topic>ANNEALING</topic><topic>BINARY ALLOY SYSTEMS</topic><topic>COMPUTERIZED SIMULATION</topic><topic>FERROMAGNETIC MATERIALS</topic><topic>IRON ALLOYS</topic><topic>MATERIALS SCIENCE</topic><topic>MIXING</topic><topic>MONTE CARLO METHOD</topic><topic>ORDER PARAMETERS</topic><topic>ORDER-DISORDER TRANSFORMATIONS</topic><topic>PLATINUM ALLOYS</topic><topic>POTENTIALS</topic><topic>TEMPERATURE DEPENDENCE</topic><topic>TEMPERATURE RANGE 0400-1000 K</topic><topic>TEMPERATURE RANGE 1000-4000 K</topic><topic>TRANSITION TEMPERATURE</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chepulskii, R. V.</creatorcontrib><creatorcontrib>Velev, J.</creatorcontrib><creatorcontrib>Butler, W. H.</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chepulskii, R. V.</au><au>Velev, J.</au><au>Butler, W. H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Monte Carlo simulation of equilibrium L1 ordering in FePt nanoparticles</atitle><jtitle>Journal of applied physics</jtitle><date>2005-05-15</date><risdate>2005</risdate><volume>97</volume><issue>10</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>First, second, and third nearest-neighbor mixing potentials for FePt alloys were calculated from first principles using the Connolly–Williams approach. Using the mixing potentials obtained in this manner, the dependency of equilibrium L10 ordering on temperature was studied for bulk and for a spherical nanoparticle with a 3.5-nm diameter at equiatomic composition by use of Monte Carlo simulation and the analytical ring approximation. The calculated order-disorder temperature for bulk (1495–1514K) was in relatively good agreement (4% error) with the experimental value (1572K). For nanoparticles of finite size, the (long-range) order parameter changed continuously from unity to zero with increasing temperature. Rather than a discontinuity indicative of a phase-transition we obtained an inflection point in the order as a function of temperature. This inflection point occurred at a temperature below the bulk phase-transition temperature and which decreased as the particle size decreased. Our calculations predict that 3.5-nm diameter particles in configurational equilibrium at 600°C (a typical annealing temperature for promoting L10 ordering) have an L10 order parameter of 0.83 (compared to a maximum possible value equal to unity). According to our investigations, the experimental absence of a (relatively) high L10 order in 3.5-nm diameter nanoparticles annealed at 600°C or below is primarily a problem of kinetics rather than equilibrium.</abstract><cop>United States</cop><doi>10.1063/1.1852351</doi></addata></record> |
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subjects | ANNEALING BINARY ALLOY SYSTEMS COMPUTERIZED SIMULATION FERROMAGNETIC MATERIALS IRON ALLOYS MATERIALS SCIENCE MIXING MONTE CARLO METHOD ORDER PARAMETERS ORDER-DISORDER TRANSFORMATIONS PLATINUM ALLOYS POTENTIALS TEMPERATURE DEPENDENCE TEMPERATURE RANGE 0400-1000 K TEMPERATURE RANGE 1000-4000 K TRANSITION TEMPERATURE |
title | Monte Carlo simulation of equilibrium L1 ordering in FePt nanoparticles |
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