Publisher's Synopsis
Excerpt from Stochastic Models for Many-Body Systems, Vol. 1: Infinite Systems in Thermal Equilibrium
In common with the true many-body Hamiltonian, our models (with one exception) are not diagonalizable by known means. However, they are sol uble in the sense that they yield formally closed integral equations for the propagators that determine the mean energies, mean occupation numbers, etc. Which are of statistical - mechanical interest. A novel feature of the models is that they contain infinite numbers of parameters whose values are chosen at random. We shall therefore call them stochastic models. The random parameters will be described in Secs. 2 and 5.
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