Conversion of magnetic anisotropy in electrodeposited Co–Ni alloy nanowires
In this paper, the influence of alternating current (ac) electrodeposition frequency and waveform is reported on chemical composition, microstructure and consequently magnetic properties of Co–Ni binary alloy nanowire arrays embedded in an alumina template. For sinusoidal and square electrodepositio...
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Veröffentlicht in: | Journal of magnetism and magnetic materials 2015-06, Vol.383, p.94-99 |
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container_title | Journal of magnetism and magnetic materials |
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creator | Samardak, A.S. Nasirpouri, F. Nadi, M. Sukovatitsina, E.V. Ognev, A.V. Chebotkevich, L.A. Komogortsev, S.V. |
description | In this paper, the influence of alternating current (ac) electrodeposition frequency and waveform is reported on chemical composition, microstructure and consequently magnetic properties of Co–Ni binary alloy nanowire arrays embedded in an alumina template. For sinusoidal and square electrodeposition waveforms the easy axis of magnetization rotates from being parallel to perpendicular orientation to nanowire long axis as the deposition frequency increases from 200 to 800Hz. The reason for the drastic change of magnetic anisotropy in nanowires is attributed to the increase of cobalt content and the crystal structure phase transformation from fcc–hcp mixture at high Ni content to hcp at high Co content. We explain the conversion of magnetic behavior of nanowire arrays in terms of a competition between the shape and magnetocrystalline anisotropies.
•Electrodeposition frequency variation leads to change of atomic percentage of Co and Ni in Co–Ni alloy nanowires.•Rising in the frequency assists to increase of Co content leading to significant changes in the crystal structure.•Rotation of the easy axis of magnetization from being parallel to the perpendicular direction to nanowire long axis is result of the competition between the magnetocrystalline and the shape magnetic anisotropies. |
doi_str_mv | 10.1016/j.jmmm.2014.10.047 |
format | Article |
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•Electrodeposition frequency variation leads to change of atomic percentage of Co and Ni in Co–Ni alloy nanowires.•Rising in the frequency assists to increase of Co content leading to significant changes in the crystal structure.•Rotation of the easy axis of magnetization from being parallel to the perpendicular direction to nanowire long axis is result of the competition between the magnetocrystalline and the shape magnetic anisotropies.</description><identifier>ISSN: 0304-8853</identifier><identifier>DOI: 10.1016/j.jmmm.2014.10.047</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Alumina template ; Arrays ; Binary alloy nanowires ; Cobalt base alloys ; Coercive force ; Conversion ; Electrodeposition ; Magnetic anisotropy ; Magnetic hysteresis ; Magnetization ; Nanowires ; Waveforms</subject><ispartof>Journal of magnetism and magnetic materials, 2015-06, Vol.383, p.94-99</ispartof><rights>2014 Elsevier B.V.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c333t-d93de0f3d0108be7dfd35c9ac6670bb5e446afca4406f84a35f450b08426a0053</citedby><cites>FETCH-LOGICAL-c333t-d93de0f3d0108be7dfd35c9ac6670bb5e446afca4406f84a35f450b08426a0053</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0304885314009585$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids></links><search><creatorcontrib>Samardak, A.S.</creatorcontrib><creatorcontrib>Nasirpouri, F.</creatorcontrib><creatorcontrib>Nadi, M.</creatorcontrib><creatorcontrib>Sukovatitsina, E.V.</creatorcontrib><creatorcontrib>Ognev, A.V.</creatorcontrib><creatorcontrib>Chebotkevich, L.A.</creatorcontrib><creatorcontrib>Komogortsev, S.V.</creatorcontrib><title>Conversion of magnetic anisotropy in electrodeposited Co–Ni alloy nanowires</title><title>Journal of magnetism and magnetic materials</title><description>In this paper, the influence of alternating current (ac) electrodeposition frequency and waveform is reported on chemical composition, microstructure and consequently magnetic properties of Co–Ni binary alloy nanowire arrays embedded in an alumina template. For sinusoidal and square electrodeposition waveforms the easy axis of magnetization rotates from being parallel to perpendicular orientation to nanowire long axis as the deposition frequency increases from 200 to 800Hz. The reason for the drastic change of magnetic anisotropy in nanowires is attributed to the increase of cobalt content and the crystal structure phase transformation from fcc–hcp mixture at high Ni content to hcp at high Co content. We explain the conversion of magnetic behavior of nanowire arrays in terms of a competition between the shape and magnetocrystalline anisotropies.
•Electrodeposition frequency variation leads to change of atomic percentage of Co and Ni in Co–Ni alloy nanowires.•Rising in the frequency assists to increase of Co content leading to significant changes in the crystal structure.•Rotation of the easy axis of magnetization from being parallel to the perpendicular direction to nanowire long axis is result of the competition between the magnetocrystalline and the shape magnetic anisotropies.</description><subject>Alumina template</subject><subject>Arrays</subject><subject>Binary alloy nanowires</subject><subject>Cobalt base alloys</subject><subject>Coercive force</subject><subject>Conversion</subject><subject>Electrodeposition</subject><subject>Magnetic anisotropy</subject><subject>Magnetic hysteresis</subject><subject>Magnetization</subject><subject>Nanowires</subject><subject>Waveforms</subject><issn>0304-8853</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp9kD1OxDAQhVOAxLJwASqXNAnjtfOzEg2K-JMWaKC2HHuCHCV2sLOLtuMO3JCT4GipqUbz5r2R3pckFxQyCrS46rJuGIZsBZRHIQNeHiULYMDTqsrZSXIaQgcQr1WxSJ5qZ3fog3GWuJYM8t3iZBSR1gQ3eTfuibEEe1Rx0Ti6YCbUpHY_X9_Phsi-d3tipXWfxmM4S45b2Qc8_5vL5O3u9rV-SDcv94_1zSZVjLEp1WumEVqmgULVYKlbzXK1lqooSmiaHDkvZKsk51C0FZcsb3kODVR8VUiAnC2Ty8Pf0buPLYZJDCYo7Htp0W2DoCWt1jynOY_W1cGqvAvBYytGbwbp94KCmHmJTsy8xMxr1iKvGLo-hDCW2Bn0IiiDVqGOLdUktDP_xX8BzDJ3-Q</recordid><startdate>20150601</startdate><enddate>20150601</enddate><creator>Samardak, A.S.</creator><creator>Nasirpouri, F.</creator><creator>Nadi, M.</creator><creator>Sukovatitsina, E.V.</creator><creator>Ognev, A.V.</creator><creator>Chebotkevich, L.A.</creator><creator>Komogortsev, S.V.</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7QF</scope><scope>7SP</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20150601</creationdate><title>Conversion of magnetic anisotropy in electrodeposited Co–Ni alloy nanowires</title><author>Samardak, A.S. ; Nasirpouri, F. ; Nadi, M. ; Sukovatitsina, E.V. ; Ognev, A.V. ; Chebotkevich, L.A. ; Komogortsev, S.V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c333t-d93de0f3d0108be7dfd35c9ac6670bb5e446afca4406f84a35f450b08426a0053</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Alumina template</topic><topic>Arrays</topic><topic>Binary alloy nanowires</topic><topic>Cobalt base alloys</topic><topic>Coercive force</topic><topic>Conversion</topic><topic>Electrodeposition</topic><topic>Magnetic anisotropy</topic><topic>Magnetic hysteresis</topic><topic>Magnetization</topic><topic>Nanowires</topic><topic>Waveforms</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Samardak, A.S.</creatorcontrib><creatorcontrib>Nasirpouri, F.</creatorcontrib><creatorcontrib>Nadi, M.</creatorcontrib><creatorcontrib>Sukovatitsina, E.V.</creatorcontrib><creatorcontrib>Ognev, A.V.</creatorcontrib><creatorcontrib>Chebotkevich, L.A.</creatorcontrib><creatorcontrib>Komogortsev, S.V.</creatorcontrib><collection>CrossRef</collection><collection>Aluminium Industry Abstracts</collection><collection>Electronics & Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of magnetism and magnetic materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Samardak, A.S.</au><au>Nasirpouri, F.</au><au>Nadi, M.</au><au>Sukovatitsina, E.V.</au><au>Ognev, A.V.</au><au>Chebotkevich, L.A.</au><au>Komogortsev, S.V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Conversion of magnetic anisotropy in electrodeposited Co–Ni alloy nanowires</atitle><jtitle>Journal of magnetism and magnetic materials</jtitle><date>2015-06-01</date><risdate>2015</risdate><volume>383</volume><spage>94</spage><epage>99</epage><pages>94-99</pages><issn>0304-8853</issn><abstract>In this paper, the influence of alternating current (ac) electrodeposition frequency and waveform is reported on chemical composition, microstructure and consequently magnetic properties of Co–Ni binary alloy nanowire arrays embedded in an alumina template. For sinusoidal and square electrodeposition waveforms the easy axis of magnetization rotates from being parallel to perpendicular orientation to nanowire long axis as the deposition frequency increases from 200 to 800Hz. The reason for the drastic change of magnetic anisotropy in nanowires is attributed to the increase of cobalt content and the crystal structure phase transformation from fcc–hcp mixture at high Ni content to hcp at high Co content. We explain the conversion of magnetic behavior of nanowire arrays in terms of a competition between the shape and magnetocrystalline anisotropies.
•Electrodeposition frequency variation leads to change of atomic percentage of Co and Ni in Co–Ni alloy nanowires.•Rising in the frequency assists to increase of Co content leading to significant changes in the crystal structure.•Rotation of the easy axis of magnetization from being parallel to the perpendicular direction to nanowire long axis is result of the competition between the magnetocrystalline and the shape magnetic anisotropies.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.jmmm.2014.10.047</doi><tpages>6</tpages></addata></record> |
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subjects | Alumina template Arrays Binary alloy nanowires Cobalt base alloys Coercive force Conversion Electrodeposition Magnetic anisotropy Magnetic hysteresis Magnetization Nanowires Waveforms |
title | Conversion of magnetic anisotropy in electrodeposited Co–Ni alloy nanowires |
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