Abstract

In the present paper both the self (or tracer) diffusion coefficient D s and the chemical (or collective) diffusion coefficient D c are computed for the Ising-Peierls lattice gas with nearest-neighbour interactions as functions of coverage θ. The two quantities are calculated in the framework of the Mori projection-operator formalism. Here D s and D c are studied for coverages up to 1 4 and memory effects are neglected. It turns out that at low lateral coupling D s depends on coverage more strongly than D c . The collective diffusion coefficient is more sensitive to the increase oflateral interactions than the self diffusion coefficient. In the range of coverages under investigation, D c is an increasing function of θ in the repulsive case, whereas, if attractive interactions are present, it decreases as θ increases. The theoretical results given by different choices of the jump dynamics are shown and briefly discussed.

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