Magnetization reversal in the pinned layer of exchange biased spin valves i
s a complex process due to the exchange interaction between the ferromagnet
ic layer and the antiferromagnetic layer. This interaction results in progr
essive reversal of the antiferromagnetic layer as the magnetization of the
ferromagnetic layer changes direction. This reversal of the antiferromagnet
will effect the subsequent reversal of the ferromagnet. It is known that t
his process is thermally activated but time dependence measurements are dif
ficult to interpret, as the exchange field is nonconstant at many positions
along the hysteresis curve. Measurements have been made of the time depend
ence of the reversal of the antiferromagnetic layer by measuring the recoil
loops, following different times spent with the ferromagnetic layer satura
ted in the negative direction. In this manner, the exchange field can be as
sumed to be constant during the reversal of the antiferromagnet. These meas
urements show a shift of the loop of the pinned layer towards positive fiel
ds. This shift in the loop is interpreted as being the result of reordering
of the antiferromagnet. Increasing the temperature during the time spent a
t saturation shows that the process is driven by thermal activation. Close
examination of the degree of loop shift with time spent at saturation shows
behavior consistent with thermal activation governed by a distribution of
activation energies. At longer times and elevated temperatures, the behavio
r of the antiferromagnet reversal suggests that this distribution is comple
x and may be multimodal. The reversal process is, however, reversible even
at high temperatures indicating that the elevated temperatures do not signi
ficantly change the structure of the ferromagnetic-antiferromagnetic layers
or the interface between them. Finally, measurements at 77 K show that the
active portion of the energy barrier distribution will change significantl
y at low temperatures. (C) 2001 American Institute of Physics.