alpha-Fe surfaces were implanted at room temperature and at 300 degrees C w
ith 50 keV Al ions with a nominal dose of 5 x 10(17) cm(-2). The samples we
re studied in the as- implanted state and after annealing at 300 degrees C.
The depth distribution of the Fe-Al phases formed was investigated nondest
ructively at RT and at 40 K by depth-selective Fe-57-conversion-electron Mo
ssbauer spectroscopy (DCEMS) in the energy range of K- as well as L-convers
ion electrons. Integral conversion-electron Mossbauer spectroscopy (CEMS) w
as performed between 30 K and RT. In addition, secondary neutral mass spect
roscopy and depth-profiling Auger-electron spectroscopy were employed for i
nvestigating the element-concentration depth profiles which were observed t
o extend deeper than Monte Carlo simulations predict. We found an atomicall
y disordered magnetic and an atomically disordered nonmagnetic bcc phase in
the as-implanted state the composition of which can be explained by the Al
-concentration dependence of bulk disordered Fe-Al alloys. After annealing
the nonmagnetic phase becomes atomically ordered (B2 structure) whereas the
magnetic phase stays in the atomically disordered state. The layer-like st
ructure of the two phases observed after annealing can be described by the
magnetic phase diagram of ordered Fe-Al alloys. (C) 1998 American Institute
of Physics. [S0021-8979(98)05524-8].