2021
DOI: 10.1007/s11669-021-00894-w
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Improving Thermodynamic Stability of SmFe12-Type Permanent Magnets from High Entropy Effect

Abstract: SmFe 12 -based compounds have been considered as one of the most promising candidates for the next generation high performance magnetic materials. SmFe 12 -based compounds exhibit excellent intrinsic hard magnetic properties with lesser amount of rare earth elements compared to other hard magnetic materials, while synthesizing bulk SmFe 12 compounds faces a big difficulty due to the thermodynamic instability of these compounds. Additional elemental doping has been attempted to stabilize SmFe 12 compounds and T… Show more

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Cited by 7 publications
(3 citation statements)
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“…mFe 12 with the tetragonal ThMn 12 structure is expected to be a candidate for the main phase of strong rare-earth permanent magnets due to favorable magnetic properties of large magnetization and a large anisotropy field that are superior to those of Nd 2 Fe 14 B at high temperatures. [1][2][3][4][5] The bulk phase of SmFe 12 is attempted to be stabilized by partial substitutions of nonmagnetic elements for Fe.…”
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“…mFe 12 with the tetragonal ThMn 12 structure is expected to be a candidate for the main phase of strong rare-earth permanent magnets due to favorable magnetic properties of large magnetization and a large anisotropy field that are superior to those of Nd 2 Fe 14 B at high temperatures. [1][2][3][4][5] The bulk phase of SmFe 12 is attempted to be stabilized by partial substitutions of nonmagnetic elements for Fe.…”
mentioning
confidence: 99%
“…[1][2][3][4][5] The bulk phase of SmFe 12 is attempted to be stabilized by partial substitutions of nonmagnetic elements for Fe. [6][7][8][9][10][11][12][13] On the other hand, to improve the performance of permanent magnets, it is necessary to design microstructures with nonmagnetic grain-boundary subphases. 5,[13][14][15][16][17][18] In fact, however, ferromagnetic bcc Fe often precipitates by substituting nonmagnetic elements for some of Fe atoms in SmFe 12 .…”
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