Abstract

The concept of the Bloch spectral function (BSF) has been extended to deal with disordered magnetic alloys with their electronic structure described using the spin polarized relativistic Korringa-Kohn-Rostoker Coherent Potential Approximation (SPR-KKR-CPA) formalism. Applications are presented for the alloy system fcc-Fe x Ni 1− x that shows a rather well defined dispersion relation and Fermi surface. Additional spin decomposition of the BSF clearly reveals the spin hybridisation due to spin-orbit coupling as well as its anisotropy in k-space.

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