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Magnetic properties of LaCo sub 13 -based systems

Journal Article · · Journal of Applied Physics; (USA)
DOI:https://doi.org/10.1063/1.344695· OSTI ID:6838225
; ; ; ;  [1]
  1. MEMS Department, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213 (USA)
Four polycomponent systems based on LaCo{sub 13} have been studied: La(Co{sub 1{minus}{ital x}}Fe{sub {ital x}}){sub 13}, La(Co{sub 1{minus}{ital x}}Al{sub {ital x}}){sub 13}, La(Co{sub 1{minus}{ital x}{minus}{ital y}}Fe{sub {ital x}}Al{sub {ital y}}){sub 13}, and La{sub 0.7}Nd{sub 0.3}(Co{sub 0.7}Fe{sub 0.3}){sub 13}. These 1:13 systems were studied because of their potential for permanent magnet fabrication. LaCo{sub 13} has a high 3{ital d} metal content, the highest for any known rare-earth intermetallic, a 13 kG saturation induction, and a high {ital T}{sub {ital c}} (1318 K). Unfortunately, it is cubic and lacks anisotropy. The substituted systems were examined as a portion of a program to find LaCo{sub 13}-based systems of applications significance. Replacement of Co in LaCo{sub 13} by Fe and/or Al leads to a rapid decline in {ital T}{sub {ital c}} for all systems studied. Replacement of Co by Al results in a decline in moment, whereas replacement by Fe leads to a rise in moment to 2.39{mu}{sub {ital B}}/3{ital d} atom for La(Co{sub 0.4}Fe{sub 0.6}){sub 13}, as compared to 2.46{mu}{sub {ital B}}/3{ital d} atom for Fe{sub 0.7}Co{sub 0.3}. Analysis of the magnetic data shows that vacancies occur in both half-bands for LaCo{sub 13} (4.8 spin up and 3.24 spin down) but in only one half-band in La(Co{sub 1{minus}{ital x}}Al{sub {ital x}}){sub 13} for {ital x}{ge}0.2. Nd in these systems carries a moment of 3{mu}{sub {ital B}}, close to that of the free tripositive ion.
OSTI ID:
6838225
Journal Information:
Journal of Applied Physics; (USA), Journal Name: Journal of Applied Physics; (USA) Vol. 67:9; ISSN 0021-8979; ISSN JAPIA
Country of Publication:
United States
Language:
English

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