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Motivation for Experiments

Above, some theoretical perspectives have been presented, on polarized electron reflection measurements of magnetic materials. This section details the motivation for undertaking the polarized electron reflection measurements on a $Co/Cu(001)$ structure, described in part III.

Colleagues at the Cavendish Laboratory had earlier performed a series of measurements on the system formed by growing a $0.5\,\mathrm{ML}$ $Mn/6\,\mathrm{ML}$ $Co/Cu(001)$ multi-layer [14,15,16]. Low-energy electron diffraction (LEED) revealed, through the existence of $(\frac{1}{2}\frac{1}{2})$ order spots, a $c(2\times{}2)$ (chessboard-like) superstructure in the plane of the film.

Three possible explanations were advanced for the $c(2\times{}2)$ superstructure [14,15,16]:

Magneto-optical Kerr effect (MOKE) measurements were taken by colleagues at the Cavendish Laboratory as part of the same project [14,15,16]. The $[110]$ direction Kerr signal was seen to increase with the addition of manganese, in the regime where the alloy exists. The immediate reaction to this is that the system's magnetic moment is increasing, i.e. that the manganese atoms that are being added are ferro-magnetically aligned, both with each other and with the cobalt. However, the simultaneous drop in $[100]$ Kerr signal did not paint the same picture, and it may be that a change in magneto-optical response, rather than a genuine addition of magnetic moments, is responsible for the increased $[110]$ signal. The possibilities are in particular need of investigation, given that a series [21,22,23] of numerical calculations, using different approximations, have produced widely differing predictions about the magnetic properties of this system.

The polarization of a reflected electron beam from the sample surface provides an alternative to MOKE, for measuring the magnetization, through the difference, for the two electron spins, in density of states at a particular energy created by the exchange splitting, and as such provides an experiment which is interesting by virtue of having an unpredictable result. The experiments presented in this thesis, using a $Co/Cu(001)$ structure, are intended as an intermediate stage on the way to similar measurements on $MnCo/Co/Cu(001)$, although they could equally well lead to similar measurements on other multi-layer structures of more direct industrial relevance, such as metal/ferromagnet or semiconductor/ferromagnet spin valves. This possibility may help to address the conclusions, concerning the motivation for experimental research projects, of statistical research the author has presented elsewhere [10].

In addition, the measurements for $Co/Cu(001)$, in themselves, allow a trial run of estimating the parameters in the new theory of this chapter, and comparing a version of that theory, in which no Weiss field affects the probing electrons, against another version, in which an adjustable Weiss field affects the probing electrons. This task is undertaken in section 5.3.

$Co/Cu(001)$ is a much-studied system. Before discussing previously published experimental polarized electron reflection results, and presenting the new, polarized electron reflection experiment, which is at the heart of this thesis, it will be as well to review other workers' published results on the structure and magnetic properties of this system.


next up previous contents
Next: Literature Review Up: Theory Previous: Classical Theory   Contents
Daniel Christopher Hatton 2004-11-30