The crystallization characteristics of glassy Cu‐Zr has been studied by differential scanning calorimetry, x‐ray diffraction, and measurement of electrical resistance and magnetic susceptibility. Our results allow us to remove many discrepancies between previously published data; they also suggest that the equiatomic Cu‐Zr does not exist as a single phase in the crystalline state. We observe parallel changes on crystallization between the magnetic susceptibility and the electrical resistance, which we interpret through changes in the d density of states.
REFERENCES
1.
R. L.
Freed
and I. B.
Vander Sande
, J. Non‐Cryst. Solids
27
, 9
(1978
).2.
A. J.
Kerns
, D. E.
Polk
, R.
Ray
, and B. C.
Giessen
, Mater. Sci. Eng.
38
, 49
(1979
).3.
4.
P. G. Zielinski, J. Ostateh, M. Kijek, and H. Matyja, in Proceedings of the 3rd International Conference on Rapidly Quenched Metals, Brighton, 1978, edited by B. Cantor (The Metals Society, London, 1978), p. 337.
5.
J. M.
Vitek
, J. B.
Vander Sande
, and N. J.
Grant
, Acta Metall.
23
, 165
, (1975
).6.
7.
Z.
Altounian
, Tu
Guohua
, and J. O.
Strom‐Olsen
, Solid State Commun.
40
, 221
(1981
).8.
Y. Calvayrac, M. Harmelin, A. Quivy, J. P. Chevalier, and J. Bigot, Proceedings of the 4th International Conference on Liquid and Amorphous Metals, Grenoble, 1980, p. 144.
9.
10.
We have observed the same phenomenon for both FeZr and NiZr at these high Zr concentrations. We are planning to examine these samples, as well as by transmission electron microscopy.
11.
12.
13.
14.
We assume that the amorphous phase is sufficiently stable to allow us to use equilibrium thermodynamics.
15.
We have tried to correlated with change in density. Unfortunately our measurements of density are not yet sufficiently accurate to allow us to draw any conclusions.
16.
T. Mizoguchi, S. von Molnar, G. S. Cargill III, T. Kudo, N. Shiotani, and H. Sekizawa, in Amorphous Magnetism II, edited by R. A. Levy and R. Hasegawa (Plenum, New York, 1977), p. 513.
17.
N. F. Mott and H. Jones, in The Theory of the Properties of Metals and Alloys (Dover, New York, 1958).
18.
P.
Oelhafen
, E.
Hauser
, H. J.
Guntherodt
, and K. H.
Bennemann
, Phys. Rev. Lett.
43
, 1134
(1978
).19.
It should also be noted that crystalline shows a saturation of resistance with temperature reminiscent of that seen in A15 compounds.
This content is only available via PDF.
© 1982 American Institute of Physics.
1982
American Institute of Physics
You do not currently have access to this content.