A comparative study on magnetostrictive strain in GdCo5 and Gd0.9Pr0.1Co5
Identifieur interne : 000A60 ( Istex/Corpus ); précédent : 000A59; suivant : 000A61A comparative study on magnetostrictive strain in GdCo5 and Gd0.9Pr0.1Co5
Auteurs : A. Amirabadizadeh ; N. Tajabor ; M. R. Alinejad ; F. PourarianSource :
- physica status solidi (c) [ 1610-1634 ] ; 2004-05.
English descriptors
Abstract
Results of the magnetostriction measurements on exchange coupled GdCo5‐type alloys, (with insignificant magnetic anisotropy of L‐quenched Gd+3 ions) show lower values compared to Gd0.9Pr0.1Co5 compound. In fact, partial substitution of Pr for Gd creates an orbital moment for the rare earth sublattice and therefore the magnetocrystalline anisotropy (MA) increases. The temperature dependence of MA introduces the spin reorientation transition in Gd0.9Pr0.1Co5 compound. Simple model calculations indicate that a negative contribution in the first order anisotropy constant (K1) appears after Pr substitution. The sign of K1 changes from negative to positive at ∼160 K with increasing temperature. The latter introduces a large increase in the anisotropic magnetostriction. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)
Url:
DOI: 10.1002/pssc.200304408
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In fact, partial substitution of Pr for Gd creates an orbital moment for the rare earth sublattice and therefore the magnetocrystalline anisotropy (MA) increases. The temperature dependence of MA introduces the spin reorientation transition in Gd0.9Pr0.1Co5 compound. Simple model calculations indicate that a negative contribution in the first order anisotropy constant (K1) appears after Pr substitution. The sign of K1 changes from negative to positive at ∼160 K with increasing temperature. The latter introduces a large increase in the anisotropic magnetostriction. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)</div></front></TEI><istex><corpusName>wiley</corpusName><author><json:item><name>A. 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The temperature dependence of MA introduces the spin reorientation transition in Gd0.9Pr0.1Co5 compound. Simple model calculations indicate that a negative contribution in the first order anisotropy constant (K1) appears after Pr substitution. The sign of K1 changes from negative to positive at ∼160 K with increasing temperature. The latter introduces a large increase in the anisotropic magnetostriction. (© 2004 WILEY‐VCH Verlag GmbH & Co. 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R.</givenNames><familyName>Alinejad</familyName></personName></creator><creator xml:id="au4" creatorRole="author" affiliationRef="#a3"><personName><givenNames>F.</givenNames><familyName>Pourarian</familyName></personName></creator></creators><affiliationGroup><affiliation xml:id="a1" countryCode="IR" type="organization"><unparsedAffiliation>Department of Physics, Faculty of Science, University of Birjand, Birjand, Iran</unparsedAffiliation></affiliation><affiliation xml:id="a2" countryCode="IR" type="organization"><unparsedAffiliation>Department of Physics, Faculty of Science, Ferdowsi University of Mashad, Mashad, Iran</unparsedAffiliation></affiliation><affiliation xml:id="a3" countryCode="US" type="organization"><unparsedAffiliation>Carnegie Mellon Institute, Carnegie Mellon University, Pittsburg, Pensylvania, 15219, USA</unparsedAffiliation></affiliation></affiliationGroup><keywordGroup xml:lang="en" type="author"><keyword xml:id="kwd1">75.30.Sg</keyword><keyword xml:id="kwd2">75.80.+q</keyword></keywordGroup><abstractGroup><abstract type="main" xml:lang="en"><title type="main">Abstract</title><p>Results of the magnetostriction measurements on exchange coupled GdCo<sub>5</sub>‐type alloys, (with insignificant magnetic anisotropy of L‐quenched Gd<sup>+3</sup> ions) show lower values compared to Gd<sub>0.9</sub>Pr<sub>0.1</sub>Co<sub>5</sub> compound. In fact, partial substitution of Pr for Gd creates an orbital moment for the rare earth sublattice and therefore the magnetocrystalline anisotropy (MA) increases. The temperature dependence of MA introduces the spin reorientation transition in Gd<sub>0.9</sub>Pr<sub>0.1</sub>Co<sub>5</sub> compound. Simple model calculations indicate that a negative contribution in the first order anisotropy constant (K<sub>1</sub>) appears after Pr substitution. The sign of K<sub>1</sub> changes from negative to positive at ∼160 K with increasing temperature. The latter introduces a large increase in the anisotropic magnetostriction. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)</p></abstract></abstractGroup></contentMeta></header></component></istex:document></istex:metadataXml><mods version="3.6"><titleInfo lang="en"><title>A comparative study on magnetostrictive strain in GdCo5 and Gd0.9Pr0.1Co5</title></titleInfo><titleInfo type="abbreviated" lang="en"><title>A Comparative study on magnetostrictive strain</title></titleInfo><titleInfo type="alternative" contentType="CDATA" lang="en"><title>A comparative study on magnetostrictive strain in GdCo5 and Gd0.9Pr0.1Co5</title></titleInfo><name type="personal"><namePart type="given">A.</namePart><namePart type="family">Amirabadizadeh</namePart><affiliation>Department of Physics, Faculty of Science, University of Birjand, Birjand, Iran</affiliation><affiliation>Department of Physics, Faculty of Science, Ferdowsi University of Mashad, Mashad, Iran</affiliation><description>Correspondence: Phone: +98 511 8438033, Fax: +98511 8405816</description><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">N.</namePart><namePart type="family">Tajabor</namePart><affiliation>Department of Physics, Faculty of Science, Ferdowsi University of Mashad, Mashad, Iran</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">M. R.</namePart><namePart type="family">Alinejad</namePart><affiliation>Department of Physics, Faculty of Science, Ferdowsi University of Mashad, Mashad, Iran</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">F.</namePart><namePart type="family">Pourarian</namePart><affiliation>Carnegie Mellon Institute, Carnegie Mellon University, Pittsburg, Pensylvania, 15219, USA</affiliation><role><roleTerm type="text">author</roleTerm></role></name><typeOfResource>text</typeOfResource><genre type="article" displayLabel="article"></genre><originInfo><publisher>WILEY‐VCH Verlag</publisher><place><placeTerm type="text">Berlin</placeTerm></place><dateIssued encoding="w3cdtf">2004-05</dateIssued><dateCaptured encoding="w3cdtf">2003-08-31</dateCaptured><dateValid encoding="w3cdtf">2003-12-31</dateValid><copyrightDate encoding="w3cdtf">2004</copyrightDate></originInfo><language><languageTerm type="code" authority="rfc3066">en</languageTerm><languageTerm type="code" authority="iso639-2b">eng</languageTerm></language><physicalDescription><internetMediaType>text/html</internetMediaType><extent unit="figures">4</extent><extent unit="references">14</extent></physicalDescription><abstract lang="en">Results of the magnetostriction measurements on exchange coupled GdCo5‐type alloys, (with insignificant magnetic anisotropy of L‐quenched Gd+3 ions) show lower values compared to Gd0.9Pr0.1Co5 compound. In fact, partial substitution of Pr for Gd creates an orbital moment for the rare earth sublattice and therefore the magnetocrystalline anisotropy (MA) increases. The temperature dependence of MA introduces the spin reorientation transition in Gd0.9Pr0.1Co5 compound. Simple model calculations indicate that a negative contribution in the first order anisotropy constant (K1) appears after Pr substitution. The sign of K1 changes from negative to positive at ∼160 K with increasing temperature. The latter introduces a large increase in the anisotropic magnetostriction. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)</abstract><subject lang="en"><genre>keywords</genre><topic>75.30.Sg</topic><topic>75.80.+q</topic></subject><relatedItem type="host"><titleInfo><title>physica status solidi (c)</title></titleInfo><titleInfo type="abbreviated"><title>phys. stat. sol. 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