Enhancement of Curie temperature of the 2 : 17 phase in nanocomposite Sm-2(Fe,Co)(15)Cr2C2/(Fe,Co) magnets

Citation
Zm. Chen et al., Enhancement of Curie temperature of the 2 : 17 phase in nanocomposite Sm-2(Fe,Co)(15)Cr2C2/(Fe,Co) magnets, J APPL PHYS, 86(7), 1999, pp. 3857-3862
Citations number
17
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
JOURNAL OF APPLIED PHYSICS
ISSN journal
00218979 → ACNP
Volume
86
Issue
7
Year of publication
1999
Pages
3857 - 3862
Database
ISI
SICI code
0021-8979(19991001)86:7<3857:EOCTOT>2.0.ZU;2-Y
Abstract
The proximity effect on the Curie temperature of exchange-coupled melt-spun nanocomposite Sm-2(Fe,Co)(15)Cr2C2/(Fe,Co) magnets consisting of a fine mi xture of hard and soft phases has been examined using thermomagnetic measur ements, x-ray diffraction (XRD), Mossbauer and transmission electron micros copic studies. A significant enhancement in the Curie temperature of the 2: 17 phase is observed in these magnets (27 degrees C in Sm2Fe15Cr2C2 and 102 degrees C in Sm2Fe11Co4Cr2C2) as compared to their patent cast alloys. XRD and Mossbauer analysis confirm that both the cast alloys and the nanocompo site magnets are comprised of the same phases [rhombohedral 2:17 and bcc Fe (Co)]. The unit cell volume of the 2:17 phase is slightly larger in ribbons and it is found to contribute to about 15% of the total Curie temperature enhancement. Microstructural studies revealed that the grain size is reduce d from 10 to 20 mu m in the cast alloy to 20-60 nm in the melt-spun magnets . The enhancement of the Curie temperature is believed to arise mainly from the exchange coupling effect between the 2:17 phase and the Fe(Co) phase w hich results in an extra exchange field at the 2:17 grains. Furthermore, th e enhancement of the Curie temperature is found to increase with the volume fraction of the Fe(Co) phase in the magnets. It is also interesting to not e that the Curie temperature of the Fe(Co) phase in the magnets remains unc hanged as compared with their parent alloys, because the exchange coupling effect disappears completely at temperature above the Curie temperature of the 2:17 phase. (C) 1999 American Institute of Physics. [S0021- 8979(99)067 19-5].