Abstract

The phase diagram of the Ising model on the simple hexagonal lattice with competing interactions is studied within the mean-field approximation. The stability analysis of a paramagnetic phase shows that the present model exhibits a Lifshitz point separating the paramagnetic phase, an antiferromagnetic phase and a modulated phase. Numerical calculations are performed to investigate a gross feature of the phase diagram. It is shown that a large number of high-order commensurate phases are stable. The resulting phase diagram is strikingly different from the corresponding phase diagram of the axial next-nearest neighbor Ising (ANNNI) model.

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