We study the Laplacian operator of an uncorrelated random network and, as an application, consider hopping processes (diffusion, random walks, signal propagation, etc.) on networks. We develop a strict approach to these problems. We derive an exact closed set of integral equations, which provide the averages of the Laplacian operator's resolvent. This enables us to describe the propagation of a signal and random walks on the network. We show that the determining parameter in this problem is the minimum degree q(m) of vertices in the network and that the high-degree part of the degree distribution is not that essential. The position of the lower edge of the Laplacian spectrum lambda(c) appears to be the same as in the regular Bethe lattice with the coordination number qm. Namely, lambda(c) > 0 if q(m) > 2, and lambda(c) = 0 if q(m) <= 2. In both of these cases the density of eigenvalues rho(lambda) --> 0 as lambda --> lambda(c) + 0, but the limiting behaviors near lambda(c) are very different. In terms of a distance from a starting vertex, the hopping propagator is a steady moving Gaussian, broadening with time. This picture qualitatively coincides with that for a regular Bethe lattice. Our analytical results include the spectral density rho(lambda) near lambda(c) and the long-time asymptotics of the autocorrelator and the propagator.
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