Diagonalization of full finite temperature Green's function by quasi-particles
arXiv:nucl-th/9304006 · doi:10.1016/0370-2693(93)91421-I
Abstract
For thermal systems, standard perturbation theory breaks down because of the absence of stable, observable asymptotic states. We show, how the introduction of {\it statistical} quasi-particles (stable, but not observable) gives rise to a consistent description. Statistical and spectral information can be cleanly separated also for interacting systems.
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