Abstract
We study the formation of local moments in a metallic host due to a localized spin-orbit (Rashba) interaction. Using the Anderson model we describe the occurrence of magnetic moments through calculation of the magnetic-non-magnetic phase transition within the mean-field scenario. We compare our results with those in the absence of the Rashba interaction. The symmetry and regime of the magnetic phase demonstrates a dependence on the above interaction. The conductance values through the impurities are also exhibited for the above phases.
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