The microstructure, high performance magnetic hardness and magnetic after-effect of an alpha- FeCo/Pr(2)Fe(14)B nanocomposite magnet with low Pr concentration.

@article{Ngo2009TheMH,
  title={The microstructure, high performance magnetic hardness and magnetic after-effect of an alpha- FeCo/Pr(2)Fe(14)B nanocomposite magnet with low Pr concentration.},
  author={Duc-The Ngo and Hong-Gam Duong and Hoang-Hai Nguyen and Chau Thi Kim Nguyen and M. A. Basith and Duc-Quang Hoang},
  journal={Nanotechnology},
  year={2009},
  volume={20 16},
  pages={
          165707
        }
}
In this paper, a systematic investigation of the microstructure, high performance magnetic hardness as well as novel magnetic memory effect of the Pr(4)Fe(76)Co(10)B(6)Nb(3)Cu(1) nanocomposite magnet fabricated by conventional melt-spinning followed by annealing at temperatures ranging from 600 to 700 degrees C in Ar gas for nanocrystallization are presented and discussed. Transmission electron microscopy (TEM) observation confirms an ultrafine structure of bcc-Fe(Co) as a magnetically soft… 

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References

SHOWING 1-10 OF 19 REFERENCES
Crystalline evolution and large coercivity in Dy-doped (Nd,Dy)2Fe14B/α-Fe nanocomposite magnets
Nanocomposite hard magnetic materials (Nd,Dy)4.5Fe77.5B18 (No. 1) and (Nd,Dy)4.5Fe76B18Nb1.2Cu0.3 (No. 2) have been prepared by crystallizing amorphous ribbons, fabricated by single roll
The effects of the thickness of magnetically hard- and soft-phase layers on magnetic properties and exchange coupling in multilayer magnets
The structure and magnetic properties of multilayer magnets containing a hard phase [HP equivalent to(Nd0.95Dy0.05)(Fe,Co,Nb,B)(5.5)] and a soft phase (SP equivalent to Fe and Fe65Co35) have been
Effect of boron on the magnetic properties and exchange-coupling effect of FePtB-type nanocomposite ribbons
Phase evolution and magnetic properties of melt-spun (Fe0.675Pt0.325)100−xBx (x=12–20) nanocomposite ribbons are investigated. For those ribbons spun at 45m∕s, followed with a 500°C isothermal
Hard magnetic properties of Fe–Co–Nd–Dy–B nanocrystalline alloys containing residual amorphous phase
The glass transition and supercooled liquid region were observed in the composition range of 4 to 56 %Co, 2 to 4 %Nd, and 18 to 30 at%B in melt-spun Fe–Co–Nd–0.5 at%Dy–B amorphous alloys. The largest
Electronic structure, exchange interactions, and Curie temperature of FeCo
Fe–Co alloys in the α phase are soft magnetic materials which have high saturation inductions over a wide range of compositions. However, above about 1250 K, an α to γ phase transition occurs. The
Nucleation fields in an exchange spring hard magnet
A detailed study of magnetization processes has been carried out on a new type of hard magnetic material. The material Nd3.8Fe73.3V3.9B18.0Si1.0 is unique among hard magnets due to the exchange
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