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The flow stress increased with the increase of aluminum content under the same deformation conditions. At high temperatures, the stress exponent was 5 and the activation energy was close to that for lattice diffusion of magnesium, whereas at low temperatures the stress exponent was 7 and activation energy was close to that for pipe diffusion for all alloys. By incorporating the effective diffusion coefficient and stacking fault energy into a constitutive equation, the dislocation creep behavior of magnesium alloys can be described by a single relation."}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381137044700581762","@type":"Researcher","foaf:name":[{"@value":"Hidetoshi Somekawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137044700581760","@type":"Researcher","foaf:name":[{"@value":"Kinji Hirai"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137044700581761","@type":"Researcher","foaf:name":[{"@value":"Hiroyuki 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Takigawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137044700581763","@type":"Researcher","foaf:name":[{"@value":"Kenji Higashi"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"09215093"}],"prism:publicationName":[{"@value":"Materials Science and Engineering: A"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"2005-10","prism:volume":"407","prism:number":"1-2","prism:startingPage":"53","prism:endingPage":"61"},"reviewed":"false","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:S0921509305006696?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:S0921509305006696?httpAccept=text/plain"}],"createdAt":"2005-08-26","modifiedAt":"2023-05-04","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360290617656505088","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Hot 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