Geodesic
Complete phase diagrams with respect to external fields at low temperatures for models with nearest-neighbor interaction in the case of a finite or countable number of ground states
Teoretičeskaâ i matematičeskaâ fizika, Tome 58 (1984) no. 2, pp. 261-278 Cet article a éte moissonné depuis la source Math-Net.Ru

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It is shown that at low temperatures and for arbitrary external fields (activities $z_k$, $\hat z=\{z_k\}$) the ensemble with the Hamiltonian (1) and particles in the set $\Phi$ is equivalent to $|\Phi|$ Ising models with activities $b_k(\hat z), \hat b(\hat z) = \{b_k(\hat z)\}$. The mapping $\hat b(\hat z)$ is a homeomorphism on the positive octant $l_\infty (\Phi)$ if $\sup\limits_k \sum\limits_{l \neq k} \exp\{-\beta\varepsilon(k,l)\}\leq \bar\psi_1$, where $\bar\psi_1$ is a small number. The pressure in the ensemble is $p(\hat z)=\sup\limits_{k \in \Phi}b_k(\hat z) = | \hat b(\hat z) |$. The limit Gibbs states corresponding to the vector $\hat z$ are small perturbations of the ground states $\alpha(x)= q \in G_1(\hat z)$ and are labeled by elements of the set $G_1(\hat z) = \{ \hat q: \ln b_q(\hat z) = p(\hat z)\}$, where the function $G_1(\hat z)$ defines the phase diagram of the ensemble. In the regions of constancy of $G_1(\hat z)$ the pressure can be continued to a holomorphie function, and the particle densities $z_l \partial p/\partial z_l$ are continuous in the closure of a region of constancy of $G_1(\hat z)$. 
@article{TMF_1984_58_2_a11,
     author = {A. G. Basuev},
     title = {Complete phase diagrams with respect to external fields at low temperatures for models with nearest-neighbor interaction in the case of a finite or countable number of ground states},
     journal = {Teoreti\v{c}eska\^a i matemati\v{c}eska\^a fizika},
     pages = {261--278},
     year = {1984},
     volume = {58},
     number = {2},
     language = {ru},
     url = {http://geodesic.mathdoc.fr/item/TMF_1984_58_2_a11/}
}
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A. G. Basuev. Complete phase diagrams with respect to external fields at low temperatures for models with nearest-neighbor interaction in the case of a finite or countable number of ground states. Teoretičeskaâ i matematičeskaâ fizika, Tome 58 (1984) no. 2, pp. 261-278. http://geodesic.mathdoc.fr/item/TMF_1984_58_2_a11/

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