Hysteresis loops of polycrystalline and single-crystal exchange biased Ni80
Fe20 (Permalloy)/ Fe50Mn50/Ni80Fe20 (Permalloy) trilayers were measured as
a function of Fe50Mn50 layer thickness with the longitudinal Kerr effect. T
he variation of the macroscopic pinning field H-p and the coercivity H-c wa
s observed over a full 360 degrees in plane rotation and Fourier analyzed.
The magnetization behavior of both Permalloy layers of the polycrystalline
samples was analyzed, and it was found that the pinning field of the bottom
layer is always greater than for the top layer, while the situation is rev
ersed for the coercivity due to defects incorporated in the antiferromagnet
ic layer. The single-crystal samples were prepared on epitaxially grown Cu(
111) on Si(110), and the magnetization behavior of the top Permalloy layer
was studied. In contrast to the polycrystalline samples, the coercivities p
eak very sharply at the easy axis, which manifests itself in large higher-o
rder Fourier coefficients. Coercivities and loop shifts show a strong linea
r dependence on the antiferromagnetic layer thickness. The relation of the
biasing direction to the crystal axes had no influence on H-c acid H-p. Thi
s behavior is attributed to complete strain relief through the buffer layer
and better crystalline growth of the trilayer as compared to the polycryst
alline samples. Examination of the results with a Ginzburg-Landau energy fu
nctional verified that the Fourier coefficients obey necessary conditions t
o achieve energetic stability together with spontaneous magnetization. The
energy functional was used to model the angular dependence of the loop shif
t.