Searcharxiv⌕ Search

arXiv subjects

R. M. Khakimov

Publications and source records attributed to R. M. Khakimov.

13 recordsLinked to original sources

Extreme Gibbs measures for a Hard-Core-SOS model on Cayley trees

We investigate splitting Gibbs measures (SGMs) of a three-state (wand-graph) hardcore SOS model on Cayley trees of order $ k \geq 2 $. Recently, this model was studied for the hinge-graph with $ k = 2, 3 $, while the case $ k \geq 4 $ remains unresolved. It was shown that as the coupling strength $θ$ increases, the number of translation-invariant SGMs (TISGMs) evolves through the sequence $ 1 \to 3 \to 5 \to 6 \to 7 $. In this paper, for wand-graph we demonstrate that for arbitrary $ k \geq 2 $, the number of TISGMs is at most three, denoted by $ μ_i $, $ i = 0, 1, 2 $. We derive the exact critical value $θ_{\text{cr}}(k)$ at which the non-uniqueness of TISGMs begins. The measure $ μ_0 $ exists for any $θ> 0$. Next, we investigate whether $ μ_i $, $i=0,1,2$ is extreme or non-extreme in the set of all Gibbs measures. The results are quite intriguing: 1) For $μ_0$: - For $ k = 2 $ and $ k = 3 $, there exist critical values $θ_1(k)$ and $θ_2(k)$ such that $ μ_0 $ is extreme if and only if $θ\in (θ_1, θ_2)$, excluding the boundary values $θ_1$ and $θ_2$, where the extremality remains undetermined. - Moreover, for $ k \geq 4 $, $ μ_0 $ is never extreme. 2) For $μ_1$ and $μ_2$ at $k=2$ there is $θ_5<θ_{\text{cr}}(2)=1$ such that these measures are extreme if $θ\in (θ_5, 1)$.

math-ph↗

Tranlation-invariant Gibbs measures for the Hard-Core model with a countable set of spin values

In this paper, we study the Hard Core (HC) model with a countable set $\mathbb Z$ of spin values on a Cayley tree of order $k=2$. This model is defined by a countable set of parameters (that is, the activity function $λ_i>0$, $i\in \mathbb Z$). A functional equation is obtained that provides the consistency condition for finite-dimensional Gibbs distributions. Analyzing this equation, the following results are obtained: Let $k\geq 2$ and $Λ=\sum_iλ_i$. For $Λ=+\infty$ there is no translation-invariant Gibbs measure (TIGM); Let $k=2$ and $Λ<+\infty$. For the model under constraint such that at $G$-admissible graph the loops are imposed at two vertices of the graph, the uniqueness of TIGM is proved; Let $k=2$ and $Λ<+\infty$. For the model under constraint such that at $G$-admissible graph the loops are imposed at three vertices of the graph, the uniqueness and non-uniqueness conditions of TIGMs are found.

math-ph↗

Periodic Gibbs measures for three-state hard-core models in the case Wand

We consider fertile three-state Hard-Core (HC) models with the activity parameter $λ>0$ on a Cayley tree. It is known that there exist four types of such models: wrench, wand, hinge, and pipe. These models arise as simple examples of loss networks with nearest-neighbor exclusion. In the case wand on a Cayley tree of order $k\geq2$, exact critical values $λ>0$ are found for which two-periodic Gibbs measures are not unique. Moreover, we study the extremality of the existing two-periodic Gibbs measures on a Cayley tree of order two.

math-ph↗

New class of Gibbs measures for two state Hard-Core model on a Cayley tree

In this paper, we consider a Hard-Core $(HC)$ model with two spin values on Cayley trees. The conception of alternative Gibbs measure is introduced and translational invariance conditions for alternative Gibbs measures are found. Also, we show that the existence of alternative Gibbs measures which are not translation-invariant. In addition, we study free energy of the model.

math.PR↗

Gibbs measures for HC-model with a countable set of spin values on a Cayley tree

In this paper, we study the HC-model with a countable set $\mathbb Z$ of spin values on a Cayley tree of order $k\geq 2$. This model is defined by a countable set of parameters (that is, the activity function $λ_i>0$, $i\in \mathbb Z$). A functional equation is obtained that provides the consistency condition for finite-dimensional Gibbs distributions. Analyzing this equation, the following results are obtained: - Let $Λ=\sum_iλ_i$. For $Λ=+\infty$ there are no translation-invariant Gibbs measures (TIGM) and no two-periodic Gibbs measures (TPGM); - For $Λ<+\infty$, the uniqueness of TIGM is proved; - Let $Λ_{\rm cr}(k)=\frac{k^k}{(k-1)^{k+1}}$. If $0<Λ\leqΛ_{\rm cr}$, then there is exactly one TPGM that is TIGM; - For $Λ>Λ_{\rm cr}$, there are exactly three TPGMs, one of which is TIGM.

math-ph↗

Weakly periodic Gibbs measures for two and three state HC models on a Cayley tree

In this paper we study two and three state HC-model on a Cayley tree. Under some conditions on parameters of the HC-model, in the case of normal divisor of the index four, we prove the existence of the weakly periodic (non periodic) Gibbs measures which are different from the known weakly periodic measures. Moreover, we find some regions for the $λ$ parameter ensuring that a extreme measure is not unique.

math-ph↗

Translation-invariant and periodic Gibbs measures for Potts model on a Cayley tree

In this paper is studied ferromagnetic three states Potts model on a Cayley tree of order three and we give explicit formulas for translation-invariant Gibbs measures. Furthermore, we show that under some conditions on the parameter of the antiferromagnetic Potts model with q-states with zero external field on the Cayley tree of order $k>2$, there are exactly 2(2^q-1) periodic (non translation-invariant) Gibbs measures.

math-ph↗

Description of the translation-invariant splitting Gibbs measures for the Potts model on a Cayley tree

For the $q$-state Potts model on a Cayley tree of order $k\geq 2$ it is well-known that at sufficiently low temperatures there are at least $q+1$ translation-invariant Gibbs measures which are also tree-indexed Markov chains. Such measures are called translation-invariant splitting Gibbs measures (TISGMs). In this paper we find all TISGMs, and show in particular that at sufficiently low temperatures their number is $2^{q}-1$. We prove that there are $[q/2]$ (where $[a]$ is the integer part of $a$) critical temperatures at which the number of TISGMs changes and give the exact number of TISGMs for each intermediate temperature. For the binary tree we give explicit formulae for the critical temperatures and the possible TISGMs. While we show that these measures are never convex combinations of each other, the question which of these measures are extremals in the set of all Gibbs measures will be treated in future work.

math-ph↗