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Physics Letters A

Order parameter for the Ising ferromagnet

Norman E. Frankel

Published Dec 1, 1968• 6 citations
Publisher
DOI
10.1016/0375-9601(68)90483-0

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The fcc spin-1 Ising (BEG) model has a dense ferromagnetic (dfdfdf) ground state instead of the ferromagnetic ground state at low temperature region and exhibits the dense ferromagnetic (dfdfdf) - ferromagnetic (FFF) phase transition for d=D/J=2.9d=D/J=2.9d=D/J=2.9, k=K/J=−0.5k=K/J=-0.5k=K/J=−0.5, ℓ=L/J=0\ell =L/J=0ℓ=L/J=0 and h=H/J=0h=H/J=0h=H/J=0. The critical behavior of the dense ferromagnetic (dfdfdf) - ferromagnetic (FFF) phase transition has been investigated using the cellular automaton cooling and heating algorithms. The universality class and the type of the dense ferromagnetic (dfdfdf) - ferromagnetic (FFF) phase transition have been researched within the framework of the finite - size scaling, the power law relations and the probability distribution. The results show that the dense ferromagnetic- ferromagnetic phase transition is of the second order and the model shows universal second order Ising critical behavior at d=2.9d=2.9d=2.9 parameter value through k=−0.5k=-0.5k=−0.5 line.