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ANNUAL REPORT - MTA SzFKI

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I. METALLURGY AND MAGNETISM<br />

L.K. Varga, I. Balogh, É. Fazakas # , P. Kamasa, G. Konczos, Gy. Kovács + , J. Pádár, L.<br />

Pogány, F.I. Tóth<br />

Metallurgy. — The bulk glass forming ability (GFA) of Cu-based alloys have been<br />

studied in collaboration with the Materials Science Department of Miskolc University,<br />

Hungary. Several compositions have been prepared, following the bulk GFA criteria<br />

published so far in the literature, such as Cu 100-x-y-z Zr x Ti y Ag z , Cu 100-x Mm x Al y where Mm<br />

means Mischmetal.<br />

Surveying all the Cu-based amorphous alloys published in the literature so far, it turned<br />

out that the atomic mismatch condition of Egami and Waseda is fulfilled for all the Cubased<br />

bulk amorphous alloys, the λ value being above 0,3. Combining the chemical<br />

coordinates of Miedema (y) with the atomic mismatch (x), the glass forming and non-glass<br />

forming regions were found separated by the following curve: y=|10|∆Φ * |-39 |∆(1/n ws 1/3 |-1|<br />

and x=|1-R x /R Cu | for the binary Cu-based alloys.<br />

The glass forming ability of Al-based alloys (mainly of Al 85 Mm 5 Ni 8 Co 2 type<br />

compositions) has been investigated during the compaction of powders obtained by gas<br />

atomising and chopping the rapidly quenched ribbons.<br />

Soft magnetic nanocrystalline alloys. — Based on a Quasi-DC hysterograph, an<br />

experimental technique has been developed to obtain the true “static” hysteresis curve.<br />

This is the so-called “ballistic “method to obtain the hysteresis loop by integrating the<br />

measured incremental permeability (µ incremental = µ diff ) versus biasing DC field, H DC . In<br />

addition, it was demonstrated that it is possible to decompose the quasi-static hysteresis<br />

loop into two contributions deriving from domain magnetization rotation (DR) and domain<br />

wall movement (DWM) (Fig. 1 and Fig. 2) and this decompositon was modelled<br />

theoretically by the hyperbolic T model. The hyperbolic T model was further improved by<br />

splitting it in 3 overlapping hysteretic contributions: one DR and two DWM (jumping and<br />

annihilation) parts. Softwares have been developed to carry out measurements of<br />

reversible magnetization at very small excitation (H ~

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