The magnetization reversal process of patterned magnetic tunnel junctions w
as investigated using finite element micromagnetics, taking into account th
e magnetostatic interactions between the pinned and the free layer. Two dif
ferent reversal modes were observed in the simulations depending on the dom
ain structure for zero applied field. In order to reduce the magnetostatic
energy, end domains form in the free layer either in the S state or the C s
tate. If the system is in the S state, the end domains grow under the influ
ence of a reversed field. The end domains touch each other, leading to the
reversal of the center. Finally, the residual domains along the edges paral
lel to the field direction reverse. If the system is in the C state, the gr
owth of the end domains leads to a four domain flux closure structure. The
domain with the magnetization in favor of the field direction expands until
the free layer becomes reversed at a field. The S state and the C state we
re found to differ in energy by less than 0.2%. (C) 2001 American Institute
of Physics.