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Sökning: onr:"swepub:oai:DiVA.org:uu-395710" > The CeFe11Ti perman...

LIBRIS Formathandbok  (Information om MARC21)
FältnamnIndikatorerMetadata
00004289naa a2200421 4500
001oai:DiVA.org:uu-395710
003SwePub
008191025s2019 | |||||||||||000 ||eng|
024a https://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-3957102 URI
024a https://doi.org/10.1088/1361-648X/ab40962 DOI
040 a (SwePub)uu
041 a engb eng
042 9 SwePub
072 7a ref2 swepub-contenttype
072 7a art2 swepub-publicationtype
100a Martinez-Casado, R.u Univ Complutense Madrid, Fac Phys Sci, Dept Mat Phys, E-28040 Madrid, Spain;Univ Torino, Dipartimento Chim, Via P Giuria 5, I-10125 Turin, Italy4 aut
2451 0a The CeFe11Ti permanent magnet :b a closer look at the microstructure of the compound
264 1b IOP PUBLISHING LTD,c 2019
338 a print2 rdacarrier
520 a High-performance permanent magnets (PM) are compounds with outstanding intrinsic magnetic properties. Most PMs are obtained from a favorable combination of rare earth metals (RE = Nd, Pr, Ce) with transition metals (TM = Fe, Co). Amongst them, CeFe11Ti claims considerable attention due to its large Curie temperature, saturation magnetization, and significant magnetocrystalline anisotropic energy. CeFe11Ti has several potential applications, in particular, in the development of electric motors for future automatic electrification. In this work, we shed some light on the mictrostructure of this compound by performing periodic hybrid-exchange density functional theory (DFT) calculations. We use a combined approach of atom-centered local orbitals, plane waves and full-potential linear muffin-tin orbital (LMTO) for our computations. The electronic configuration of the atoms involved in different steps of formation of the crystal structure of CeFe11Ti gives an explanation on the effect of Ce and Ti on its magnetic properties. While Ti stabilizes the structure, atomic orbitals of Ce hybridizes with Fe atomic orbitals to a significant extent and alters the electronic bands. Our calculations confirm a valence of 3(+) for Ce, which has been deemed crucial to obtain a large magnetocrystalline anisotropy. In addition, we analyze several spin configurations, with the ferromagnetic configuration being most stable. We compare and contrast our data to those available and provide an insight for further development of optimized high-performance PMs. Moreover, we compute the Magnetocrystalline Anisotropy of this compound by means of two approaches: the Force Theorem and a full-potential LMTO method.
650 7a NATURVETENSKAPx Fysikx Den kondenserade materiens fysik0 (SwePub)103042 hsv//swe
650 7a NATURAL SCIENCESx Physical Sciencesx Condensed Matter Physics0 (SwePub)103042 hsv//eng
653 a electronic structure
653 a permanent magnets
653 a magnetic properties
700a Dasmahapatra, A.u Univ Torino, Dipartimento Chim, Via P Giuria 5, I-10125 Turin, Italy4 aut
700a Sgroi, M. F.u Ctr Ric FIAT, Str Torino 50, I-10043 Orbassano, TO, Italy4 aut
700a Romero-Muniz, C.u Univ Autonoma Madrid, Dept Fis Teor Mat Condensada, E-28049 Madrid, Spain4 aut
700a Herper, Heike C.u Uppsala universitet,Materialteori4 aut0 (Swepub:uu)heihe597
700a Vekilova, Olga Yu.u Uppsala universitet,Materialteori4 aut0 (Swepub:uu)olgve867
700a Ferrari, A. M.u Univ Torino, Dipartimento Chim, Via P Giuria 5, I-10125 Turin, Italy;Univ Turin, Ctr Excellence, NIS, Turin, Italy4 aut
700a Pullini, D.u Ctr Ric FIAT, Str Torino 50, I-10043 Orbassano, TO, Italy4 aut
700a Desmarais, J.u Univ Torino, Dipartimento Chim, Via P Giuria 5, I-10125 Turin, Italy4 aut
700a Maschio, L.u Univ Torino, Dipartimento Chim, Via P Giuria 5, I-10125 Turin, Italy;Univ Turin, Ctr Excellence, NIS, Turin, Italy4 aut
710a Univ Complutense Madrid, Fac Phys Sci, Dept Mat Phys, E-28040 Madrid, Spain;Univ Torino, Dipartimento Chim, Via P Giuria 5, I-10125 Turin, Italyb Univ Torino, Dipartimento Chim, Via P Giuria 5, I-10125 Turin, Italy4 org
773t Journal of Physicsd : IOP PUBLISHING LTDg 31:50q 31:50x 0953-8984x 1361-648X
8564 8u https://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-395710
8564 8u https://doi.org/10.1088/1361-648X/ab4096

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