We rewrite the exact expression for the finite temperature two-point correlation function for the magnetization as a partition function of some field theory. This removes singularities and provides a convenient form to develop a virial expansion (the expansion in powers of soliton density).To calculate correlation functions in strongly correlated systems is not an easy task, even if the corresponding models happen to be integrable. For models with dynamically generated spectral gaps the most powerful technique is the formfactor approach pioneered by Karowski et. al.[1] and perfected by Smirnov [2]. This approach works wonderfully for zero temperature, but encounters difficulties at T = 0. These difficulties are related to singularities in the operator matrix elements (formfactors). These singularities exist for operators nonlocal with respect to solitons, they originate from forward scattering processes and their treatment requires careful infrared regularization. Despite long efforts a correct regularization has not been yet found. However, for models of free fermions (such as the XY model or the Quantum Ising model), there are alternative means to calculate the correlation functions which allow to bypass the above problems. These alternative approaches include the determinant representation of the correlation functions [3], [4] and the semiclassical method [5] (which may have much wider application, see [6], [7]). For these results to have a greater use one has to establish their relationship with the formfactor approach. A step in this direction was made in [8] where the semiclassical results [5], [6], [7] were reproduced by summing up the leading singularities in the formfactor expansion. Such summation was restricted to the leading order in the soliton density n ∼ exp(−M/T ) (M is the spectral gap). In this paper we describe a formfactor-based representation for correlation functions which, though in its present form is valid only for models of free fermions, is rather suggestive and may give rise to useful generalizations in the future. For the Quantum Ising (QI) model, which is the main object of this paper, this procedure naturally gives rise to a virial expansion of the dynamical spin susceptibility.
The QI model Hamiltonian is