Abstract

Mixed spin-1/2 and spin-1 Ising ferrimagnets on a triangular lattice with sublattices A, B, and C are studied for two spin-value distributions (S(A),S(B),S(C))=(1/2,1/2,1) and (1/2,1,1) by Monte Carlo simulations. The nonbipartite character of the lattice induces geometrical frustration in both systems, which leads to the critical behavior rather different from their ferromagnetic counterparts. We confirm second-order phase transitions belonging to the standard Ising universality class occurring at higher temperatures, however, in both models these change at tricritical points (TCP) to first-order transitions at lower temperatures. In the model (1/2,1/2,1), TCP occurs on the boundary between paramagnetic and ferrimagnetic (±1/2,±1/2,∓1) phases. The boundary between two ferrimagnetic phases (±1/2,±1/2,∓1) and (±1/2,∓1/2,0) at lower temperatures is always first order and it is joined by a line of second-order phase transitions between the paramagnetic and the ferrimagnetic (±1/2,∓1/2,0) phases at a critical endpoint. The tricritical behavior is also confirmed in the model (1/2,1,1) on the boundary between the paramagnetic and ferrimagnetic (0,±1,∓1) phases.

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