Competition between direct exchange and indirect RKKY coupling in Fe/V[001] superlattices
Fe 10 Å /V t V (001) superlattices are prepared by magnetron sputter deposition and characterized using x-ray diffraction (XRD), magneto-optical Kerr effect (MOKE) magnetometry, and x-ray magnetic circular dichroism (XMCD). MOKE loops show three peaks in saturation field as a function of t V , indic...
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Veröffentlicht in: | IEEE transactions on magnetics 1998-07, Vol.34 (4), p.864-866 |
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creator | Harp, G.R. Schwickert, M.M. Tomaz, M.A. Tao Lin Lederman, D. Mayo, E. O'Brien, W.L. |
description | Fe 10 Å /V t V (001) superlattices are prepared by magnetron sputter deposition and characterized using x-ray diffraction (XRD), magneto-optical Kerr effect (MOKE) magnetometry, and x-ray magnetic circular dichroism (XMCD). MOKE loops show three peaks in saturation field as a function of t V , indicating RKKY induced AF coupling at t V =22 Å, 32 Å, and 42 Å. The expected AF coupling peak at 12 Å, however, is missing. XMCD measurements show that the V layers carry a relatively large magentic moment which extends surprisingly far from the Fe/V interface. Such 'transient ferromagentism' suggests a strong V-V direct exchange coupling within the V layer. We argue that the V-V direct exchange coupling suppresses the 12 Å AF coupling peak, but since direct exchange coupling decays more quickly than RKKY coupling, the AF peaks at 22, 32, and 42 Å are observed. |
doi_str_mv | 10.1109/20.706293 |
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MOKE loops show three peaks in saturation field as a function of t V , indicating RKKY induced AF coupling at t V =22 Å, 32 Å, and 42 Å. The expected AF coupling peak at 12 Å, however, is missing. XMCD measurements show that the V layers carry a relatively large magentic moment which extends surprisingly far from the Fe/V interface. Such 'transient ferromagentism' suggests a strong V-V direct exchange coupling within the V layer. We argue that the V-V direct exchange coupling suppresses the 12 Å AF coupling peak, but since direct exchange coupling decays more quickly than RKKY coupling, the AF peaks at 22, 32, and 42 Å are observed.</description><identifier>ISSN: 0018-9464</identifier><identifier>EISSN: 1941-0069</identifier><identifier>DOI: 10.1109/20.706293</identifier><identifier>CODEN: IEMGAQ</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Applied sciences ; Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Exact sciences and technology ; Iron ; Kerr effect ; Magnetic field measurement ; Magnetic moments ; Magnetic properties and materials ; Magnetic properties of monolayers and thin films ; Magnetic properties of surface, thin films and multilayers ; Magnetic superlattices ; Magnetooptic effects ; Metals. Metallurgy ; Physics ; Saturation magnetization ; Sputtering ; X-ray diffraction ; X-ray scattering</subject><ispartof>IEEE transactions on magnetics, 1998-07, Vol.34 (4), p.864-866</ispartof><rights>1998 INIST-CNRS</rights><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c306t-7db1bb0ee4c916d860aca72f82c8adece201fc6e845318282975c45f5d108ab73</citedby><cites>FETCH-LOGICAL-c306t-7db1bb0ee4c916d860aca72f82c8adece201fc6e845318282975c45f5d108ab73</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/706293$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>309,310,314,780,784,789,790,796,23929,23930,25139,27923,27924,54757</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/706293$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=2426641$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Harp, G.R.</creatorcontrib><creatorcontrib>Schwickert, M.M.</creatorcontrib><creatorcontrib>Tomaz, M.A.</creatorcontrib><creatorcontrib>Tao Lin</creatorcontrib><creatorcontrib>Lederman, D.</creatorcontrib><creatorcontrib>Mayo, E.</creatorcontrib><creatorcontrib>O'Brien, W.L.</creatorcontrib><title>Competition between direct exchange and indirect RKKY coupling in Fe/V[001] superlattices</title><title>IEEE transactions on magnetics</title><addtitle>TMAG</addtitle><description>Fe 10 Å /V t V (001) superlattices are prepared by magnetron sputter deposition and characterized using x-ray diffraction (XRD), magneto-optical Kerr effect (MOKE) magnetometry, and x-ray magnetic circular dichroism (XMCD). MOKE loops show three peaks in saturation field as a function of t V , indicating RKKY induced AF coupling at t V =22 Å, 32 Å, and 42 Å. The expected AF coupling peak at 12 Å, however, is missing. XMCD measurements show that the V layers carry a relatively large magentic moment which extends surprisingly far from the Fe/V interface. Such 'transient ferromagentism' suggests a strong V-V direct exchange coupling within the V layer. We argue that the V-V direct exchange coupling suppresses the 12 Å AF coupling peak, but since direct exchange coupling decays more quickly than RKKY coupling, the AF peaks at 22, 32, and 42 Å are observed.</description><subject>Applied sciences</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Exact sciences and technology</subject><subject>Iron</subject><subject>Kerr effect</subject><subject>Magnetic field measurement</subject><subject>Magnetic moments</subject><subject>Magnetic properties and materials</subject><subject>Magnetic properties of monolayers and thin films</subject><subject>Magnetic properties of surface, thin films and multilayers</subject><subject>Magnetic superlattices</subject><subject>Magnetooptic effects</subject><subject>Metals. Metallurgy</subject><subject>Physics</subject><subject>Saturation magnetization</subject><subject>Sputtering</subject><subject>X-ray diffraction</subject><subject>X-ray scattering</subject><issn>0018-9464</issn><issn>1941-0069</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1998</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNo9kMFLwzAUh4MoOKcHr55yEMFDtyRN0_Qow6lsIIgKQ6Sk6euMdGlNUtT_3krLTo_33vf7Dj-EzimZUUqyOSOzlAiWxQdoQjNOI0JEdogmhFAZZVzwY3Ti_We_8oSSCdosml0LwQTTWFxA-AawuDQOdMDwoz-U3QJWtsTGjten1WqDddO1tbHb_oyXMH9964Xv2HctuFqFYDT4U3RUqdrD2Tin6GV5-7y4j9aPdw-Lm3WkYyJClJYFLQoCwHVGRSkFUVqlrJJMS1WCBkZopQVInsRUMsmyNNE8qZKSEqmKNJ6iq8HbuuarAx_ynfEa6lpZaDqf95FYyDTpwesB1K7x3kGVt87slPvNKcn_y8sZyYfyevZylCqvVV05ZbXx-wDjTAhOe-xiwAwA7L-j4w84LXYa</recordid><startdate>19980701</startdate><enddate>19980701</enddate><creator>Harp, G.R.</creator><creator>Schwickert, M.M.</creator><creator>Tomaz, M.A.</creator><creator>Tao Lin</creator><creator>Lederman, D.</creator><creator>Mayo, E.</creator><creator>O'Brien, W.L.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><scope>RIA</scope><scope>RIE</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>19980701</creationdate><title>Competition between direct exchange and indirect RKKY coupling in Fe/V[001] superlattices</title><author>Harp, G.R. ; Schwickert, M.M. ; Tomaz, M.A. ; Tao Lin ; Lederman, D. ; Mayo, E. ; O'Brien, W.L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c306t-7db1bb0ee4c916d860aca72f82c8adece201fc6e845318282975c45f5d108ab73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1998</creationdate><topic>Applied sciences</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Exact sciences and technology</topic><topic>Iron</topic><topic>Kerr effect</topic><topic>Magnetic field measurement</topic><topic>Magnetic moments</topic><topic>Magnetic properties and materials</topic><topic>Magnetic properties of monolayers and thin films</topic><topic>Magnetic properties of surface, thin films and multilayers</topic><topic>Magnetic superlattices</topic><topic>Magnetooptic effects</topic><topic>Metals. Metallurgy</topic><topic>Physics</topic><topic>Saturation magnetization</topic><topic>Sputtering</topic><topic>X-ray diffraction</topic><topic>X-ray scattering</topic><toplevel>online_resources</toplevel><creatorcontrib>Harp, G.R.</creatorcontrib><creatorcontrib>Schwickert, M.M.</creatorcontrib><creatorcontrib>Tomaz, M.A.</creatorcontrib><creatorcontrib>Tao Lin</creatorcontrib><creatorcontrib>Lederman, D.</creatorcontrib><creatorcontrib>Mayo, E.</creatorcontrib><creatorcontrib>O'Brien, W.L.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>IEEE transactions on magnetics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Harp, G.R.</au><au>Schwickert, M.M.</au><au>Tomaz, M.A.</au><au>Tao Lin</au><au>Lederman, D.</au><au>Mayo, E.</au><au>O'Brien, W.L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Competition between direct exchange and indirect RKKY coupling in Fe/V[001] superlattices</atitle><jtitle>IEEE transactions on magnetics</jtitle><stitle>TMAG</stitle><date>1998-07-01</date><risdate>1998</risdate><volume>34</volume><issue>4</issue><spage>864</spage><epage>866</epage><pages>864-866</pages><issn>0018-9464</issn><eissn>1941-0069</eissn><coden>IEMGAQ</coden><abstract>Fe 10 Å /V t V (001) superlattices are prepared by magnetron sputter deposition and characterized using x-ray diffraction (XRD), magneto-optical Kerr effect (MOKE) magnetometry, and x-ray magnetic circular dichroism (XMCD). MOKE loops show three peaks in saturation field as a function of t V , indicating RKKY induced AF coupling at t V =22 Å, 32 Å, and 42 Å. The expected AF coupling peak at 12 Å, however, is missing. XMCD measurements show that the V layers carry a relatively large magentic moment which extends surprisingly far from the Fe/V interface. Such 'transient ferromagentism' suggests a strong V-V direct exchange coupling within the V layer. We argue that the V-V direct exchange coupling suppresses the 12 Å AF coupling peak, but since direct exchange coupling decays more quickly than RKKY coupling, the AF peaks at 22, 32, and 42 Å are observed.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/20.706293</doi><tpages>3</tpages></addata></record> |
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subjects | Applied sciences Condensed matter: electronic structure, electrical, magnetic, and optical properties Exact sciences and technology Iron Kerr effect Magnetic field measurement Magnetic moments Magnetic properties and materials Magnetic properties of monolayers and thin films Magnetic properties of surface, thin films and multilayers Magnetic superlattices Magnetooptic effects Metals. Metallurgy Physics Saturation magnetization Sputtering X-ray diffraction X-ray scattering |
title | Competition between direct exchange and indirect RKKY coupling in Fe/V[001] superlattices |
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