Abstract

The magnetic domain structure of near stoichiometric (Nd 11.8Fe 82.3B 5.9) nanocrystalline alloy ribbon has been examined using magnetic force microscopy (MFM) as a function of processing conditions. Amorphous structured ribbons of Nd 2Fe 14B with an average thickness of 25 μm were produced by chill block melt-spinning. Subsequently, samples were heat treated at 600°C for 4 min to produce a nanocrystalline structure consisting of Nd 2Fe 14B grains of average size ∼35 nm. These were compared to ribbons of the same composition, but melt spun directly to the nanocrystalline state, also with an average grain size of ∼35 nm. MFM imaging was undertaken using CoCr, NiFe and Fe/SiO 2 coated pyramidal Si tips. The as-cast amorphous ribbons exhibited weak magnetic contrast with a correlation length of 130±20 nm, but with a small elongation in one direction, as shown by Fourier transforms of the MFM images. Nanocrystalline samples produced by devitrification exhibited longer correlation lengths of 1000±50 nm and with a stronger angular component to the Fourier transform. The application of a 5 T field to the nanophase sample in a direction normal to the sample plane resulted in a reduction of the correlation length to 600±50 nm and a reduction in the directionality of the magnetic contrast. However, the application of a 5 T field in the plane of the ribbon resulted in an elongation of the contrast in a direction parallel to the applied field, irrespective of the in-plane field direction. In contrast, ribbon melt spun directly to a nanocrystalline structure exhibited a uniform Fourier transform both in the as-cast and remanent states. The length scale of dominant magnetic structure was 350±30 nm for the as-cast and 620±30 nm for the remanent state. Within the dominant magnetic structure, a finer structure was apparent, of a scale comparable to the grain size.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call