Ganikhodjaev Nasir - Academia.edu (original) (raw)
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Papers by Ganikhodjaev Nasir
In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and ... more In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and only if the associated Markov process satisfies one.
In this paper we investigate extreme Gibbs measures with period p for the Vannimenus model.
Linear Algebra and Its Applications, 2006
In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and ... more In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and only if the associated Markov process satisfies one.
Journal of Statistical Physics, 2009
We study the phase diagram for Potts model on a Cayley tree with competing nearest-neighbor inter... more We study the phase diagram for Potts model on a Cayley tree with competing nearest-neighbor interactions J 1, prolonged next-nearest-neighbor interactions J p and one-level next-nearest-neighbor interactions J o . Vannimenus proved that the phase diagram of Ising model with J o =0 contains a modulated phase, as found for similar models on periodic lattices, but the multicritical Lifshitz point is at zero temperature. Later Mariz et al. generalized this result for Ising model with J o ≠0 and recently Ganikhodjaev et al. proved similar result for the three-state Potts model with J o =0. We consider Potts model with J o ≠0 and show that for some values of J o the multicritical Lifshitz point be at non-zero temperature. We also prove that as soon as the same-level interactionJ o is nonzero, the paramagnetic phase found at high temperatures for J o =0 disappears, while Ising model does not obtain such property. To perform this study, an iterative scheme similar to that appearing in real space renormalization group frameworks is established; it recovers, as particular case, previous work by Ganikhodjaev et al. for J o =0. At vanishing temperature, the phase diagram is fully determined for all values and signs of J 1,J p and J o . At finite temperatures several interesting features are exhibited for typical values of J o /J 1.
Abstract One of the main problems of the Statistical Physics is to describe all Gibbs measures co... more Abstract One of the main problems of the Statistical Physics is to describe all Gibbs measures corresponding to the given Hamiltonian. It is well known that such measures form a nonempty convex compact subset in the set of all probabilistic measures. The purpose ...
In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and ... more In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and only if the associated Markov process satisfies one.
Journal of Statistical Mechanics-theory and Experiment, 2011
One of the main problems of statistical physics is that of describing all Gibbs measures correspo... more One of the main problems of statistical physics is that of describing all Gibbs measures corresponding to a given Hamiltonian. It is well known that such measures form a nonempty convex compact subset in the set of all probability measures. The purpose of this paper is to investigate extreme Gibbs measures of the Vannimenus model.
In this paper we investigate extreme Gibbs measures with period p for the Vannimenus model.
Journal of Statistical Mechanics-theory and Experiment, 2011
One of the main problems of statistical physics is that of describing all Gibbs measures correspo... more One of the main problems of statistical physics is that of describing all Gibbs measures corresponding to a given Hamiltonian. It is well known that such measures form a nonempty convex compact subset in the set of all probability measures. The purpose of this paper is to investigate extreme Gibbs measures of the Vannimenus model.
Journal of Statistical Physics, 2009
We study the phase diagram for Potts model on a Cayley tree with competing nearest-neighbor inter... more We study the phase diagram for Potts model on a Cayley tree with competing nearest-neighbor interactions J 1, prolonged next-nearest-neighbor interactions J p and one-level next-nearest-neighbor interactions J o . Vannimenus proved that the phase diagram of Ising model with J o =0 contains a modulated phase, as found for similar models on periodic lattices, but the multicritical Lifshitz point is at zero temperature. Later Mariz et al. generalized this result for Ising model with J o ≠0 and recently Ganikhodjaev et al. proved similar result for the three-state Potts model with J o =0. We consider Potts model with J o ≠0 and show that for some values of J o the multicritical Lifshitz point be at non-zero temperature. We also prove that as soon as the same-level interactionJ o is nonzero, the paramagnetic phase found at high temperatures for J o =0 disappears, while Ising model does not obtain such property. To perform this study, an iterative scheme similar to that appearing in real space renormalization group frameworks is established; it recovers, as particular case, previous work by Ganikhodjaev et al. for J o =0. At vanishing temperature, the phase diagram is fully determined for all values and signs of J 1,J p and J o . At finite temperatures several interesting features are exhibited for typical values of J o /J 1.
Abstract One of the main problems of the Statistical Physics is to describe all Gibbs measures co... more Abstract One of the main problems of the Statistical Physics is to describe all Gibbs measures corresponding to the given Hamiltonian. It is well known that such measures form a nonempty convex compact subset in the set of all probabilistic measures. The purpose ...
In this paper a notion of entropy transmission of quantum channels is introduced as a natural ext... more In this paper a notion of entropy transmission of quantum channels is introduced as a natural extension of Ohya's entropy. Here by quantum channel is meant unital completely positive mappings (ucp) of B(H)B(H)B(H) into itself, where HHH is an infinite dimensional Hilbert space. Using a representation theorem of ucp mapping we associate to every ucp map a uniquely determined state,
Linear Algebra and Its Applications, 2006
In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and ... more In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and only if the associated Markov process satisfies one.
In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and ... more In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and only if the associated Markov process satisfies one.
In this paper we investigate extreme Gibbs measures with period p for the Vannimenus model.
Linear Algebra and Its Applications, 2006
In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and ... more In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and only if the associated Markov process satisfies one.
Journal of Statistical Physics, 2009
We study the phase diagram for Potts model on a Cayley tree with competing nearest-neighbor inter... more We study the phase diagram for Potts model on a Cayley tree with competing nearest-neighbor interactions J 1, prolonged next-nearest-neighbor interactions J p and one-level next-nearest-neighbor interactions J o . Vannimenus proved that the phase diagram of Ising model with J o =0 contains a modulated phase, as found for similar models on periodic lattices, but the multicritical Lifshitz point is at zero temperature. Later Mariz et al. generalized this result for Ising model with J o ≠0 and recently Ganikhodjaev et al. proved similar result for the three-state Potts model with J o =0. We consider Potts model with J o ≠0 and show that for some values of J o the multicritical Lifshitz point be at non-zero temperature. We also prove that as soon as the same-level interactionJ o is nonzero, the paramagnetic phase found at high temperatures for J o =0 disappears, while Ising model does not obtain such property. To perform this study, an iterative scheme similar to that appearing in real space renormalization group frameworks is established; it recovers, as particular case, previous work by Ganikhodjaev et al. for J o =0. At vanishing temperature, the phase diagram is fully determined for all values and signs of J 1,J p and J o . At finite temperatures several interesting features are exhibited for typical values of J o /J 1.
Abstract One of the main problems of the Statistical Physics is to describe all Gibbs measures co... more Abstract One of the main problems of the Statistical Physics is to describe all Gibbs measures corresponding to the given Hamiltonian. It is well known that such measures form a nonempty convex compact subset in the set of all probabilistic measures. The purpose ...
In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and ... more In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and only if the associated Markov process satisfies one.
Journal of Statistical Mechanics-theory and Experiment, 2011
One of the main problems of statistical physics is that of describing all Gibbs measures correspo... more One of the main problems of statistical physics is that of describing all Gibbs measures corresponding to a given Hamiltonian. It is well known that such measures form a nonempty convex compact subset in the set of all probability measures. The purpose of this paper is to investigate extreme Gibbs measures of the Vannimenus model.
In this paper we investigate extreme Gibbs measures with period p for the Vannimenus model.
Journal of Statistical Mechanics-theory and Experiment, 2011
One of the main problems of statistical physics is that of describing all Gibbs measures correspo... more One of the main problems of statistical physics is that of describing all Gibbs measures corresponding to a given Hamiltonian. It is well known that such measures form a nonempty convex compact subset in the set of all probability measures. The purpose of this paper is to investigate extreme Gibbs measures of the Vannimenus model.
Journal of Statistical Physics, 2009
We study the phase diagram for Potts model on a Cayley tree with competing nearest-neighbor inter... more We study the phase diagram for Potts model on a Cayley tree with competing nearest-neighbor interactions J 1, prolonged next-nearest-neighbor interactions J p and one-level next-nearest-neighbor interactions J o . Vannimenus proved that the phase diagram of Ising model with J o =0 contains a modulated phase, as found for similar models on periodic lattices, but the multicritical Lifshitz point is at zero temperature. Later Mariz et al. generalized this result for Ising model with J o ≠0 and recently Ganikhodjaev et al. proved similar result for the three-state Potts model with J o =0. We consider Potts model with J o ≠0 and show that for some values of J o the multicritical Lifshitz point be at non-zero temperature. We also prove that as soon as the same-level interactionJ o is nonzero, the paramagnetic phase found at high temperatures for J o =0 disappears, while Ising model does not obtain such property. To perform this study, an iterative scheme similar to that appearing in real space renormalization group frameworks is established; it recovers, as particular case, previous work by Ganikhodjaev et al. for J o =0. At vanishing temperature, the phase diagram is fully determined for all values and signs of J 1,J p and J o . At finite temperatures several interesting features are exhibited for typical values of J o /J 1.
Abstract One of the main problems of the Statistical Physics is to describe all Gibbs measures co... more Abstract One of the main problems of the Statistical Physics is to describe all Gibbs measures corresponding to the given Hamiltonian. It is well known that such measures form a nonempty convex compact subset in the set of all probabilistic measures. The purpose ...
In this paper a notion of entropy transmission of quantum channels is introduced as a natural ext... more In this paper a notion of entropy transmission of quantum channels is introduced as a natural extension of Ohya's entropy. Here by quantum channel is meant unital completely positive mappings (ucp) of B(H)B(H)B(H) into itself, where HHH is an infinite dimensional Hilbert space. Using a representation theorem of ucp mapping we associate to every ucp map a uniquely determined state,
Linear Algebra and Its Applications, 2006
In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and ... more In the paper we prove that a quadratic stochastic process satisfies the ergodic principle if and only if the associated Markov process satisfies one.