K. Fukamichi et al., ATOMIC STRUCTURES, MAGNETOVOLUME AND PRESSURE EFFECTS IN AMORPHOUS LA(FEXAL1-X)(13) ALLOYS CONSISTING OF ICOSAHEDRAL CLUSTERS, Science Reports of the Research Institutes, Tohoku University, Series A: Physics, Chemistry, and Metallurgy, 41(1), 1995, pp. 9-40
Citations number
138
Categorie Soggetti
Material Science","Metallurgy & Metallurigical Engineering
The atomic structures of amorphous La(FexAl1-x)(13) alloys have been i
nvestigated by x-ray diffraction, and the local ordering characterized
by the icosahedral clusters has been confirmed. From the Fe-57 Mossba
uer spectra, it has been revealed that the local environment around Fe
atoms in the amorphous La(Fe0.90Al0.10)(13) alloy is very similar to
that in the crystalline counterpart. Re-entrant spin-glass behavior ha
s been observed in the concentration range where the antiferromagnetic
order occurs in the crystalline state. The Curie temperature in the a
morphous state decreases with increasing x and it is higher than the N
eel and Curie temperatures in the crystalline state. The spin-wave sti
ffness constant in the amorphous state is extremely small, suggesting
a magnetic instability. The amorphous RE(Fe1-xAlx)(13) alloys also exh
ibit re-entrant spin-glass behavior and the spin freezing temperature
is hardly changed by replacing RE because there is no change in the Fe
-Fe distance in the icosahedral clusters. A large thermal expansion an
omaly has been observed in a wide temperature range. This anomaly is r
etained, even at high temperatures well above T-c. A significant Delta
E effect has also been found in the temperature and field dependences
of Young's modulus. The temperature dependence of the forced-volume m
agnetostriction partial derivative omega/partial derivative H exhibits
a broad peak at the spin freezing temperature T-f and its divergent b
ehavior at T-f is accounted for by the variable amplitude of the local
magnetic moment in the itinerant spin glasses. The temperature depend
ence of the saturation magnetostriction lambda(S) of the ferromagnetic
alloys is explained by the two-ion model, reflecting the peculiar amo
rphous structure consisting of icosahedral clusters. Poisson's ratio d
etermined from the surface phase velocities of the Rayleigh and Sezawa
waves is very close to 1/3. The compressibility kappa obtained from B
rillouin scattering is significantly large. Various magnetovolume and
pressure effects become remarkable with increasing Fe content.