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Auger electrons from magnetically ordered solids are spin polarized. As an example ferromagnetic Fe₈₃{B}₁₇$ glass was studied. The polarization of the Fe Auger electrons exhibits structures on the order of 20%, both parallel and opposite to the magnetization of the sample depending on the particular transition. Auger electrons from B are unpolarized. The technique opens new perspectives in the study of magnetic solids, particularly alloys and compounds.
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Landolt et al. (1982) studied this question.
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