Branch Cuts Due to Finite-Temperature Quasiparticles

Abstract

The branch points of individual thermal self-energy diagrams at $k^2=4m^2,k^2=9m^2,...$ are shown not to be branch points of the full thermal self-energy. Branch points of the full theory are determined by the complex, temperature-dependent energies of the quasiparticles, defined as the pole location, $k_0=\mathcal{E}(\vec{k})$, of the exact retarded propagator. The full retarded self-energy is found to have branch points at $k_0=2\mathcal{E}(\vec{k}/2)$ and $k_0=3\mathcal{E}(\vec{k}/3)$ as well as cuts in the space-like region. The discontinuities across the branch cuts are complex. The advanced self-energy is related by reflection to the retarded.

31 pages, Revtex

References in corpus (2)

• Finite-temperature reaction-rate formula: Finite volume system, detailed balance, $T\to 0$ limit, and cutting rules
• Heat Bath Particle Number Spectrum

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