Abstract

We studied damage spreading in a Driven Lattice Gas (DLG) model as a function of the temperature TT, the magnitude of the external driving field EE, and the lattice size. The DLG model undergoes an order-disorder second-order phase transition at the critical temperature Tc(E)T_c(E), such that the ordered phase is characterized by high-density strips running along the direction of the applied field; while in the disordered phase one has a lattice-gas-like behaviour. It is found that the damage always spreads for all the investigated temperatures and reaches a saturation value DsatD_{sat} that depends only on TT. DsatD_{sat} increases for T<Tc(E=∞)T<T_c(E=\infty), decreases for T>Tc(E=∞)T>T_c(E=\infty) and is free of finite-size effects. This behaviour can be explained as due to the existence of interfaces between the high-density strips and the lattice-gas-like phase whose roughness depends on TT. Also, we investigated damage spreading for a range of finite fields as a function of TT, finding a behaviour similar to that of the case with E=∞E=\infty.

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