This paper is a continuation of a recent one in which, apparently for the first time, the
existence of polaritons in ionic crystals was proven in a microscopic electrodynamic
theory. This was obtained through an explicit computation of the dispersion curves. Here
the main further contribution consists in studying electric susceptibility, from which the
spectrum can be inferred. We show how susceptibility is obtained by the Green-Kubo methods
of Hamiltonian statistical mechanics, and give for it a concrete expression in terms of
time-correlation functions. As in the previous paper, here too we work in a completely
classical framework, in which the electrodynamic forces acting on the charges are all
taken into account, both the retarded forces and the radiation reaction ones. So, in order
to apply the methods of statistical mechanics, the system has to be previously reduced to
a Hamiltonian one. This is made possible in virtue of two global properties of classical
electrodynamics, namely, the Wheeler-Feynman identity and the Ewald resummation
properties, the proofs of which were already given for ordered system. The second
contribution consists in formulating the theory in a completely general way, so that in
principle it applies also to disordered systems such as glasses, or liquids or gases,
provided the two general properties mentioned above continue to hold. A first step in this
direction is made here by providing a completely general proof of the Wheeler-Feynman
identity, which is shown to be the counterpart of a general causality property of
classical electrodynamics. Finally it is shown how a line spectrum can appear at all in
classical systems, as a counterpart of suitable stability properties of the motions, with
a broadening due to a coexistence of chaoticity. The relevance of some recent results of
the theory of dynamical systems in this connection is also pointed out.