Iron-rich amorphous alloys with nonmagnetic transition metals (TM) or
rare-earth (RE) metals show a rich variety of complex spin-structures
that have been described as spin-glass-like, spero- or asperomagnetic.
Amorphous Fe-Y alloys have attracted particular attention because it
has been suggested that, in contrast to other amorphous Fe-TM and Fe-R
E alloys showing re-entrant spin-glass behaviour, in Fe-Y alloys the s
pin-glass transition could occur directly from the paramagnetic phase.
It has also been suggested that, unlike most other alloys where the s
pin-glass-like phase is restricted to high Fe concentrations, amorphou
s Fe-Y alloys are noncollinear at all compositions. We have recently p
resented a technique for a selfconsistent calculation of noncollinear
spin-structures in crystalline and amorphous alloys based on a tight-b
inding-Hubbard Hamiltonian generated via a canonical transformation of
the local-spin-density (LSD) Hamiltonian. This approach has been used
to analyze the magnetic properties of amorphous Fe-Y alloys. We show
that, unlike, for example, amorphous Fe-Zr alloys where the net magnet
ization is well defined in the spin-glass and in the ferromagnetic pha
ses and independent of the initialization of the magnetic structure, f
or Fe-Y energetically nearly degenerate low- and high-moment phases ca
n be induced by different initializations. This could explain the obse
rved strong dependence of the magnetic state on the preparation of the
amorphous phase and its strong variation under applied external field
s or pressures.