{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1363670320478074880.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1063/1.4754123"}},{"identifier":{"@type":"URI","@value":"https://pubs.aip.org/aip/apl/article-pdf/doi/10.1063/1.4754123/13585116/132410_1_online.pdf"}}],"dc:title":[{"@value":"Magnetic and electronic properties of <i>D</i>22-Mn3Ge (001) films"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>Oriented thin films of Mn3Ge with the tetragonal D022 structure, grown on strontium titanate substrates, exhibit a low magnetization Ms = 73 kA m−1 combined with high uniaxial anisotropy Ku = 0.91 MJ m−3 at 300 K, making them potentially useful for thermally stable sub-10 nm spin torque memory elements. The highly ordered epitaxial Mn3Ge (001) films show 46% diffusive spin polarization at the Fermi level, measured by point contact Andreev reflection. Density functional calculations show that the compounds are ferrimagnetic, with anisotropic spin polarization at the Fermi level.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380004233536446855","@type":"Researcher","foaf:name":[{"@value":"H. Kurt"}],"jpcoar:affiliationName":[{"@value":"School of Physics and CRANN, Trinity College , Dublin 2, Ireland"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670320478074753","@type":"Researcher","foaf:name":[{"@value":"N. Baadji"}],"jpcoar:affiliationName":[{"@value":"School of Physics and CRANN, Trinity College , Dublin 2, Ireland"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670320478074752","@type":"Researcher","foaf:name":[{"@value":"K. Rode"}],"jpcoar:affiliationName":[{"@value":"School of Physics and CRANN, Trinity College , Dublin 2, Ireland"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670320478074755","@type":"Researcher","foaf:name":[{"@value":"M. Venkatesan"}],"jpcoar:affiliationName":[{"@value":"School of Physics and CRANN, Trinity College , Dublin 2, Ireland"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670320478074880","@type":"Researcher","foaf:name":[{"@value":"P. Stamenov"}],"jpcoar:affiliationName":[{"@value":"School of Physics and CRANN, Trinity College , Dublin 2, Ireland"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670320478074882","@type":"Researcher","foaf:name":[{"@value":"S. Sanvito"}],"jpcoar:affiliationName":[{"@value":"School of Physics and CRANN, Trinity College , Dublin 2, Ireland"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670320478074754","@type":"Researcher","foaf:name":[{"@value":"J. M. D. 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