Abstract
AbstractThe possibility is investigated of a spin‐glass state as the ground state of a binary Ising magnet AB which is characterized (in the nearest neighbour approximation) by the competitive exchange interactions: IAA > 0; IAB > 0; IBB > 0. It is shown that due to increase of the antiferromagnetic component B concentration c in an intermediate concentration region either a spin‐glass state occurs or the first‐order phase transition from a random ferromagnetic state into a random antiferromagnetic one occurs depending upon exchange parameter ratios and crystal lattice type.
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