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Thermodynamics of fully connected Blume-Emery-Griffiths neural networks  [PDF]
D. Bolle,T. Verbeiren
Physics , 2002, DOI: 10.1088/0305-4470/36/2/301
Abstract: The thermodynamic and retrieval properties of fully connected Blume-Emery-Griffiths networks, storing ternary patterns, are studied using replica mean-field theory. Capacity-temperature phase diagrams are derived for several values of the pattern activity. It is found that the retrieval phase is the largest in comparison with other three-state neuron models. Furthermore, the meaning and stability of the so-called quadrupolar phase is discussed as a function of both the temperature and the pattern activity. Where appropriate, the results are compared with the diluted version of the model.
Dynamics and thermodynamics of the spherical frustrated Blume-Emery-Griffiths model  [PDF]
A. Caiazzo,A. Coniglio,M. Nicodemi
Physics , 2003, DOI: 10.1103/PhysRevE.66.046101
Abstract: We introduce a spherical version of the frustrated Blume-Emery-Griffiths model and solve exactly the statics and the Langevin dynamics for zero particle-particle coupling (K=0). In this case the model exhibits an equilibrium transition from a disordered to a spin glass phase which is always continuous for nonzero temperature. The same phase diagram results from the study of the dynamics. Furthermore, we notice the existence of a nonequilibrium time regime in a region of the disordered phase, characterized by aging as occurs in the spin glass phase. Due to a finite equilibration time, the system displays in this region the pattern of interrupted aging.
The Blume-Emery-Griffiths neural network: dynamics for arbitrary temperature  [PDF]
D. Bolle,J. Busquets Blanco,G. M. Shim,T. Verbeiren
Physics , 2003, DOI: 10.1016/S0378-4371(03)00629-0
Abstract: The parallel dynamics of the fully connected Blume-Emery-Griffiths neural network model is studied for arbitrary temperature. By employing a probabilistic signal-to-noise approach, a recursive scheme is found determining the time evolution of the distribution of the local fields and, hence, the evolution of the order parameters. A comparison of this approach is made with the generating functional method, allowing to calculate any physical relevant quantity as a function of time. Explicit analytic formula are given in both methods for the first few time steps of the dynamics. Up to the third time step the results are identical. Some arguments are presented why beyond the third time step the results differ for certain values of the model parameters. Furthermore, fixed-point equations are derived in the stationary limit. Numerical simulations confirm our theoretical findings.
Time evolution of the extremely diluted Blume-Emery-Griffiths neural network  [PDF]
D. Bolle',D. R. C. Dominguez,R. Erichsen Jr.,E. Korutcheva,W. K. Theumann
Physics , 2002, DOI: 10.1103/PhysRevE.68.062901
Abstract: The time evolution of the extremely diluted Blume-Emery-Griffiths neural network model is studied, and a detailed equilibrium phase diagram is obtained exhibiting pattern retrieval, fluctuation retrieval and self-sustained activity phases. It is shown that saddle-point solutions associated with fluctuation overlaps slow down considerably the flow of the network states towards the retrieval fixed points. A comparison of the performance with other three-state networks is also presented.
Parallel dynamics of the fully connected Blume-Emery-Griffiths neural network  [PDF]
D. Bolle,J. Busquets Blanco,G. M. Shim
Physics , 2002, DOI: 10.1016/S0378-4371(02)01528-5
Abstract: The parallel dynamics of the fully connected Blume-Emery-Griffiths neural network model is studied at zero temperature for arbitrary using a probabilistic approach. A recursive scheme is found determining the complete time evolution of the order parameters, taking into account all feedback correlations. It is based upon the evolution of the distribution of the local field, the structure of which is determined in detail. As an illustrative example, explicit analytic formula are given for the first few time steps of the dynamics. Furthermore, equilibrium fixed-point equations are derived and compared with the thermodynamic approach. The analytic results find excellent confirmation in extensive numerical simulations.
The Blume-Emery-Griffiths Spin Glass Model  [PDF]
Mauro Sellitto,Mario Nicodemi,Jeferson J. Arenzon
Physics , 1997, DOI: 10.1051/jp1:1997197
Abstract: We study the equilibrium properties of the Blume-Emery-Griffiths model with bilinear quenched disorder in the case of attractive as well as repulsive biquadratic interactions. The global phase diagram of the system is calculated in the context of the replica symmetric mean field approximation.
Phase coexistence and relaxation of the spherical frustrated Blume-Emery-Griffiths model with attractive particles coupling  [PDF]
A. Caiazzo,A. Coniglio,M. Nicodemi
Physics , 2003, DOI: 10.1209/epl/i2003-10080-8
Abstract: We study the equilibrium and dynamical properties of a spherical version of the frustrated Blume-Emery-Griffiths model at mean field level for attractive particle-particle coupling (K>0). Beyond a second order transition line from a paramagnetic to a (replica symmetric) spin glass phase, the density-temperature phase diagram is characterized by a tricritical point from which, interestingly, a first order transition line starts with coexistence of the two phases. In the Langevin dynamics the paramagnetic/spin glass discontinuous transition line is found to be dependent on the initial density; close to this line, on the paramagnetic side, the correlation-response plot displays interrupted aging.
Blume-Emery-Griffiths Model in a Random Transverse Field  [PDF]
H. Ez-Zahraouy,H. Mahboub,A. Benyoussef,M. J. Ouazzani
Physics , 2004,
Abstract: The effect of the random quantum transverse field $\Omega$ on the tricritical behavior of the spin-1 Blume- Emery- Griffiths (BEG) model is studied using effective field theory. It is found, that the tricritical behavior depends on both the biquadratic interaction $K$, single- ion anisotropy $\Delta$, and the concentration $p$ of the disorder of $\Omega$. Indeed, there exist a special value $p_{1}$ of the probability $p$ below which the tricritical behavior disappears.
Optimal Capacity of the Blume-Emery-Griffiths perceptron  [PDF]
D. Bolle,I. Perez Castillo,G. M. Shim
Physics , 2002, DOI: 10.1103/PhysRevE.67.036113
Abstract: A Blume-Emery-Griffiths perceptron model is introduced and its optimal capacity is calculated within the replica-symmetric Gardner approach, as a function of the pattern activity and the imbedding stability parameter. The stability of the replica-symmetric approximation is studied via the analogue of the Almeida-Thouless line. A comparison is made with other three-state perceptrons.
The Blume-Emery-Griffiths Spin Glass and Inverted Tricritical Points  [PDF]
V. Ongun ?z?elik,A. Nihat Berker
Physics , 2008, DOI: 10.1103/PhysRevE.78.031104
Abstract: The Blume-Emery-Griffiths spin glass is studied by renormalization-group theory in d=3. The boundary between the ferromagnetic and paramagnetic phases has first-order and two types of second-order segments. This topology includes an inverted tricritical point, first-order transitions replacing second-order transitions as temperature is lowered. The phase diagrams show disconnected spin-glass regions, spin-glass and paramagnetic reentrances, and complete reentrance, where the spin-glass phase replaces the ferromagnet as temperature is lowered for all chemical potentials.
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