“…As noticed in the Introduction we resort to the use of NESEF. According to the formalism, following Mori, Zwanzig and others [31,32,33,34,35,36], the Hamiltonian of the system under consideration is separated out in a so-called relevant partĤ 0 , consisting of the energy operators of the free degrees of freedom, andĤ ′ containing the interactions among them and the coupling with external sources and reservoirs. In our case herê…”