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We show that the spectral function for single-particle excitations in a two-dimensional Fermi liquid has a Lorentzian shape in the low-energy limit. Landau quasiparticles have a uniquely defined spectral weight and a decay rate which is much smaller than the quasiparticle energy. By contrast, perturbation theory and the T-matrix approximation yield spurious deviations from Fermi-liquid behavior, which are particularly pronounced for a linearized dispersion relation.
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Halboth et al. (1998) studied this question.
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