It is shown that the ferromagnetic Ising model on a Cayley tree lattice exhibits a new type of phase transition at the field $B=0$ below the Bethe-Peierls transition temperature TBP. The leading nonanalytic part of the free energy is of the form B^κ, where the "critical" exponent κ(T) increases smoothly from one to infinity as the temperature goes from 0 to TBP. This implies a transition of "continuous" order κ.
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Müller‐Hartmann et al. (1974) studied this question.
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