Abstract

We consider a linear Hamiltonian system consisting of a classical particle and a scalar field describing by the wave or Klein–Gordon equations with variable coefficients. The initial data of the system are supposed to be a random function which has some mixing properties. We study the distribution μ t of the random solution at time moments t ∈ R. The main result is the convergence of μ t to a Gaussian probability measure as t→∞. The application to the case of Gibbs initial measures is given.

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