Magnetic interactions in nanocrystalline SmFeCo
D.R. Cornejo, F.P. Missell, J. M. González
Abstract
D.R. Cornejo, F.P. Missell, J. M. González
Abstract
Several samples of enhanced-remanence nanocrystalline Sm15Fe19Co66 were prepared by mechanical alloying of the elementary powders followed by heat treatments. Sample A had a remanence ratio η=σr/σs=0.68 and Hc=7.1 kOe, while, for B, η=0.58 and Hc=10.4 kOe, and, for C, η=0.57 and Hc=12.6 kOe. The isothermal remanent magnetization Mr(H), obtained for different initial demagnetized states (ac, dc+, dc−), and the demagnetization remanence Md(−H), obtained for an initially saturated state, were determined. The ac-demagnetization Henkel plot showed both magnetizing and demagnetizing interactions as observed in other nanocrystalline magnets. A comparison with the moving Preisach model indicates the importance of both mean-field and random interactions.
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Several samples of enhanced-remanence nanocrystalline Sm15Fe19Co66 were prepared by mechanical alloying of the elementary powders followed by heat treatments. Sample A had a remanence ratio η=σr/σs=0.68 and Hc=7.1 kOe, while, for B, η=0.58 and Hc=10.4 kOe, and, for C, η=0.57 and Hc=12.6 kOe. The isothermal remanent magnetization Mr(H), obtained for different initial demagnetized states (ac, dc+, dc−), and the demagnetization remanence Md(−H), obtained for an initially saturated state, were determined. The ac-demagnetization Henkel plot showed both magnetizing and demagnetizing interactions as observed in other nanocrystalline magnets. A comparison with the moving Preisach model indicates the importance of both mean-field and random interactions.
Key concepts: Remanence, Nanocrystalline material, Demagnetizing field, Materials science, Condensed matter physics, Isothermal process, Stoner–Wohlfarth model, Magnetization