Magnetic properties and anisotropic coercivity in nanogranular films of Co/Al sub(2)O sub(3) above the percolation limit
Magnetic properties of nanogranular ferromagnetic Co/Al sub(2)O sub(3) films with 74.5 at% Co, which is above the percolation limit, are investigated. It is established that the films have perpendicular magnetic anisotropy and a weaker in-plane anisotropy. The magnetization curves show that the film...
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Veröffentlicht in: | Journal of physics. D, Applied physics Applied physics, 2014-08, Vol.47 (34), p.1-10 |
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creator | Kulyk, M M Kalita, V M Lozenko, A F Ryabchenko, S M Stognei, O V Sitnikov, A V Korenivski, V |
description | Magnetic properties of nanogranular ferromagnetic Co/Al sub(2)O sub(3) films with 74.5 at% Co, which is above the percolation limit, are investigated. It is established that the films have perpendicular magnetic anisotropy and a weaker in-plane anisotropy. The magnetization curves show that the film consists of two magnetic components: a dominating contribution from magneto-anisotropic isolated grains with the anisotropy axis perpendicular to the film plane and a weaker contribution from the percolated part of the film. This two-component magnetic composition of the films, with the dominating contribution from the nanograins, is confirmed by transmission electron microscopy as well as by ferromagnetic resonance spectroscopy. It is further established that the coercive field of the film is almost entirely determined by the percolated part of the film. In this, the angular dependence of the coercive force, H sub(c)([straighttheta] sub()H, is essentially proportional to sin super(-1)[straighttheta] sub()H where [straighttheta] sub()His the angle between the applied field and the film's normal. However, for [straighttheta] sub()H arrow right O, H sub(c)([straighttheta] sub()H there is a narrow minimum with H sub(c) approaching zero. Such non-linear dependence agrees well with our modelling results for a two-component magnetic system of the film, where the non-percolated nanograins have a distinct perpendicular anisotropy. The reported results should be important for in-depth characterization and understanding the magnetism and anisotropy in inhomogeneous systems as well as for applications, specifically in perpendicular magnetic recording. |
doi_str_mv | 10.1088/0022-3727/47/34/345002 |
format | Article |
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It is established that the films have perpendicular magnetic anisotropy and a weaker in-plane anisotropy. The magnetization curves show that the film consists of two magnetic components: a dominating contribution from magneto-anisotropic isolated grains with the anisotropy axis perpendicular to the film plane and a weaker contribution from the percolated part of the film. This two-component magnetic composition of the films, with the dominating contribution from the nanograins, is confirmed by transmission electron microscopy as well as by ferromagnetic resonance spectroscopy. It is further established that the coercive field of the film is almost entirely determined by the percolated part of the film. In this, the angular dependence of the coercive force, H sub(c)([straighttheta] sub()H, is essentially proportional to sin super(-1)[straighttheta] sub()H where [straighttheta] sub()His the angle between the applied field and the film's normal. However, for [straighttheta] sub()H arrow right O, H sub(c)([straighttheta] sub()H there is a narrow minimum with H sub(c) approaching zero. Such non-linear dependence agrees well with our modelling results for a two-component magnetic system of the film, where the non-percolated nanograins have a distinct perpendicular anisotropy. The reported results should be important for in-depth characterization and understanding the magnetism and anisotropy in inhomogeneous systems as well as for applications, specifically in perpendicular magnetic recording.</description><identifier>ISSN: 0022-3727</identifier><identifier>EISSN: 1361-6463</identifier><identifier>DOI: 10.1088/0022-3727/47/34/345002</identifier><language>eng</language><subject>Aluminum oxide ; Anisotropy ; Coercive force ; Magnetic properties ; Magnetization curves ; Nanostructure ; Nonlinearity ; Percolation</subject><ispartof>Journal of physics. D, Applied physics, 2014-08, Vol.47 (34), p.1-10</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,778,782,27911,27912</link.rule.ids></links><search><creatorcontrib>Kulyk, M M</creatorcontrib><creatorcontrib>Kalita, V M</creatorcontrib><creatorcontrib>Lozenko, A F</creatorcontrib><creatorcontrib>Ryabchenko, S M</creatorcontrib><creatorcontrib>Stognei, O V</creatorcontrib><creatorcontrib>Sitnikov, A V</creatorcontrib><creatorcontrib>Korenivski, V</creatorcontrib><title>Magnetic properties and anisotropic coercivity in nanogranular films of Co/Al sub(2)O sub(3) above the percolation limit</title><title>Journal of physics. D, Applied physics</title><description>Magnetic properties of nanogranular ferromagnetic Co/Al sub(2)O sub(3) films with 74.5 at% Co, which is above the percolation limit, are investigated. It is established that the films have perpendicular magnetic anisotropy and a weaker in-plane anisotropy. The magnetization curves show that the film consists of two magnetic components: a dominating contribution from magneto-anisotropic isolated grains with the anisotropy axis perpendicular to the film plane and a weaker contribution from the percolated part of the film. This two-component magnetic composition of the films, with the dominating contribution from the nanograins, is confirmed by transmission electron microscopy as well as by ferromagnetic resonance spectroscopy. It is further established that the coercive field of the film is almost entirely determined by the percolated part of the film. In this, the angular dependence of the coercive force, H sub(c)([straighttheta] sub()H, is essentially proportional to sin super(-1)[straighttheta] sub()H where [straighttheta] sub()His the angle between the applied field and the film's normal. However, for [straighttheta] sub()H arrow right O, H sub(c)([straighttheta] sub()H there is a narrow minimum with H sub(c) approaching zero. Such non-linear dependence agrees well with our modelling results for a two-component magnetic system of the film, where the non-percolated nanograins have a distinct perpendicular anisotropy. The reported results should be important for in-depth characterization and understanding the magnetism and anisotropy in inhomogeneous systems as well as for applications, specifically in perpendicular magnetic recording.</description><subject>Aluminum oxide</subject><subject>Anisotropy</subject><subject>Coercive force</subject><subject>Magnetic properties</subject><subject>Magnetization curves</subject><subject>Nanostructure</subject><subject>Nonlinearity</subject><subject>Percolation</subject><issn>0022-3727</issn><issn>1361-6463</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNqNT01LAzEUDKJgrf4FybE9rM1LdpPdYyl-QaWX3kuSTWokTeomW_TfG1Q8CzMMzBuGeQjdArkD0rYLQiitmKBiUYsFqwuaYp2hCTAOFa85O0eTv9AlukrpjRDS8BYm6ONF7oPJTuPjEI9myM4kLENf6FLMxSsnHc2g3cnlT-wCDjLE_SDD6OWArfOHhKPFq7hYepxGNaPzzbeyOZYqngzOrwaXah29zC4G7N3B5Wt0YaVP5uZXp2j7cL9dPVXrzePzarmujrysVwCgBJO9AsUaKkVjG2U0U2C1say1FmyrO6563huhCGVEWtmB5qApcMOmaPZTW957H03Ku4NL2ngvg4lj2gEXousEqeEfUdqxmresZl8xcHC3</recordid><startdate>20140830</startdate><enddate>20140830</enddate><creator>Kulyk, M M</creator><creator>Kalita, V M</creator><creator>Lozenko, A F</creator><creator>Ryabchenko, S M</creator><creator>Stognei, O V</creator><creator>Sitnikov, A V</creator><creator>Korenivski, V</creator><scope>7QQ</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20140830</creationdate><title>Magnetic properties and anisotropic coercivity in nanogranular films of Co/Al sub(2)O sub(3) above the percolation limit</title><author>Kulyk, M M ; Kalita, V M ; Lozenko, A F ; Ryabchenko, S M ; Stognei, O V ; Sitnikov, A V ; Korenivski, V</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p661-b111b73adb1b352a75f5bec3b1fcef38ff1f8c96bd6de7b0230afa91c61c216e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Aluminum oxide</topic><topic>Anisotropy</topic><topic>Coercive force</topic><topic>Magnetic properties</topic><topic>Magnetization curves</topic><topic>Nanostructure</topic><topic>Nonlinearity</topic><topic>Percolation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kulyk, M M</creatorcontrib><creatorcontrib>Kalita, V M</creatorcontrib><creatorcontrib>Lozenko, A F</creatorcontrib><creatorcontrib>Ryabchenko, S M</creatorcontrib><creatorcontrib>Stognei, O V</creatorcontrib><creatorcontrib>Sitnikov, A V</creatorcontrib><creatorcontrib>Korenivski, V</creatorcontrib><collection>Ceramic Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of physics. D, Applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kulyk, M M</au><au>Kalita, V M</au><au>Lozenko, A F</au><au>Ryabchenko, S M</au><au>Stognei, O V</au><au>Sitnikov, A V</au><au>Korenivski, V</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Magnetic properties and anisotropic coercivity in nanogranular films of Co/Al sub(2)O sub(3) above the percolation limit</atitle><jtitle>Journal of physics. D, Applied physics</jtitle><date>2014-08-30</date><risdate>2014</risdate><volume>47</volume><issue>34</issue><spage>1</spage><epage>10</epage><pages>1-10</pages><issn>0022-3727</issn><eissn>1361-6463</eissn><abstract>Magnetic properties of nanogranular ferromagnetic Co/Al sub(2)O sub(3) films with 74.5 at% Co, which is above the percolation limit, are investigated. It is established that the films have perpendicular magnetic anisotropy and a weaker in-plane anisotropy. The magnetization curves show that the film consists of two magnetic components: a dominating contribution from magneto-anisotropic isolated grains with the anisotropy axis perpendicular to the film plane and a weaker contribution from the percolated part of the film. This two-component magnetic composition of the films, with the dominating contribution from the nanograins, is confirmed by transmission electron microscopy as well as by ferromagnetic resonance spectroscopy. It is further established that the coercive field of the film is almost entirely determined by the percolated part of the film. In this, the angular dependence of the coercive force, H sub(c)([straighttheta] sub()H, is essentially proportional to sin super(-1)[straighttheta] sub()H where [straighttheta] sub()His the angle between the applied field and the film's normal. However, for [straighttheta] sub()H arrow right O, H sub(c)([straighttheta] sub()H there is a narrow minimum with H sub(c) approaching zero. Such non-linear dependence agrees well with our modelling results for a two-component magnetic system of the film, where the non-percolated nanograins have a distinct perpendicular anisotropy. The reported results should be important for in-depth characterization and understanding the magnetism and anisotropy in inhomogeneous systems as well as for applications, specifically in perpendicular magnetic recording.</abstract><doi>10.1088/0022-3727/47/34/345002</doi><tpages>10</tpages></addata></record> |
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subjects | Aluminum oxide Anisotropy Coercive force Magnetic properties Magnetization curves Nanostructure Nonlinearity Percolation |
title | Magnetic properties and anisotropic coercivity in nanogranular films of Co/Al sub(2)O sub(3) above the percolation limit |
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