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Magnetic Properties of Nd-Fe-B-M (M=Si, C) Bulk Nanocomposite Magnets Prepared by the Spark Plasma Sintering Method

Published online by Cambridge University Press:  26 February 2011

Tomokazu Fukuzaki
Affiliation:
[email protected], Tokyo University of Sicence, Polyscale Technology Research Center, 2641, Ymazaki, Noda-shi, Chiba-ken, 278-8510, Japan
Keisuke Tanaka
Affiliation:
[email protected], Tokyo University of Science, Department of Materials Science and Technology, 2641, Yamazaki, Noda-shi, Chiba-ken, 278-8510, Japan
Kazue Nishimoto
Affiliation:
[email protected], Tokyo University of Science, Department of Materials Science and Technology, 2641, Yamazaki, Noda-shi, Chiba-ken, 278-8510, Japan
Yuji Muro
Affiliation:
[email protected], Tokyo University of Science, Department of Physics, 2641, Yamazaki, Noda-shi, Chiba-ken, 278-8510, Japan
Keishi Nishio
Affiliation:
[email protected], Tokyo University of Science, Department of Materials Science and Technology, 2641, Yamazaki, Noda-shi, Chiba-ken, 278-8510, Japan
Ryuji Tamura
Affiliation:
[email protected], Tokyo University of Science, Department of Materials Science and Technology, 2641, Yamazaki, Noda-shi, Chiba-ken, 278-8510, Japan
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Abstract

We have prepared Nd2Fe14B/Fe3B bulk nanocomposite magnets at the compositions of Nd4Fe77.5B18.5-xMx (M=Si, C) by substitution of other elements M for B. For the sample substituted with 1 at.%Si and sintered at 600 oC, the coercivity exhibits the highest value of 227 kA/m. It has also been found that the grain sizes of the Nd2Fe14B and the Fe3B phases depend on the ramp-up time and the reduction of the grain size leads to an increase of the coercivity. On the other hand, the samples substituted with C exhibit soft magnetic behaviors, which is attributed to the suppression of the precipitation of the Nd2Fe14B hard magnetic phase.

Type
Research Article
Copyright
Copyright © Materials Research Society 2008

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