• Nenhum resultado encontrado

Braz. J. Phys. vol.38 número1

N/A
N/A
Protected

Academic year: 2018

Share "Braz. J. Phys. vol.38 número1"

Copied!
5
0
0

Texto

Loading

Imagem

TABLE I: Values of ρ 0 , when occurs ρ ∞ > 0.5 for the first time, for different values of T , for a system with z = 8 (without  self-interaction) and z = 9 (with self-interaction).
FIG. 6: Phase diagram of ρ ∞ in the parameter space. (a) z = 8 and z = 9, contours of the cooperative/defective phase; (b) z = 8 and z = 9, contours of the cooperative/coexistence/defective phase; (c) z = 20 and z = 19, contours of the cooperative/defectiv
FIG. 7: Phase diagram of ρ ∞ in the parameter space. (a) contours of the cooperative/defective phase for even z = (4,6,8,12,16,20) (without self-interaction); (b) contours of the cooperative/defective phase for odd z = (5,7,9,13, 17,19) (with self-interact

Referências

Documentos relacionados

As com- pared with other classes of models with long-range couplings, such as the random band matrix model and models with long- range couplings and pure diagonal disorder, the

(The choice of a lower energy bound is important because with too low a value the histogram never becomes sufficiently flat.) In some continuous models the ground state energy is

We have used a connection with the Standard Mapping near a transition from local to global chaos and found the position of these two invariant spanning curves limiting the size of

It is easy to see that the phase space for this version of the model presents a large number of attracting fixed points (sinks), whose orbits are plotted in different colours.. We

For such a regime, the model exhibits a route to chaos known as period doubling and we obtain a constant along the bifurcations so called the Feigenbaum’s number δ.. Keywords:

In doing this, it is explored the entrance/encapsulation and subsequent oscillatory mechanism of the capsule within the nanotube, determination of the equilibrium position of

8: This figure shows the noise effects (left plot) and temperature effects (right plot) in the density of motivated players using the Gibbs sampling dynamics.. Considering here also

We review some computer algorithms for the simulation of off-lattice clusters grown from a seed, with empha- sis on the diffusion-limited aggregation, ballistic aggregation and