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Q. Tao,1 T. Ouisse,2 D. Pinek,2 O. Chaix-Pluchery,2 F. Wilhelm,3 A. Rogalev,3 C. Opagiste,4 L. Jouffret,5 A. Champagne,6 J.-C. Charlier,6 J. Lu,1 L. Hultman,1 M. W. Barsoum,7 and J. Rosen1 1Thin Film Physics, Department of Physics, Chemistry and Biology (IFM), Linköping University, SE-581 83 Linköping, Sweden 2Université Grenoble-Alpes, CNRS, Grenoble INP, LMGP, F-38000 Grenoble, France 3European Synchrotron Radiation Facility (ESRF), CS40220, F-38043 Grenoble Cedex 9, France 4Université Grenoble-Alpes, CNRS, Institut NEEL, Grenoble INP, F-38000 Grenoble, France 5Institut de Chimie de Clermont Ferrand, F-63178 Aubière, France 6Institute of Condensed Matter and Nanosciences, UCLouvain, B-1348 Louvain-la-Neuve, Belgium 7Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA

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Rare-earth (RE) nanolaminates <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Mo</mml:mi><mml:mn>4</mml:mn></mml:msub><mml:msub><mml:mi>RE</mml:mi><mml:mn>4</mml:mn></mml:msub><mml:msub><mml:mi>Al</mml:mi><mml:mn>7</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">C</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:math> featuring ferromagnetism and mixed-valence states

Rare-earth (RE) nanolaminates Mo4RE4Al7C3 featuring ferromagnetism and mixed-valence states