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The influence of the electron-phonon interaction on the electronic spectral properties in a two-dimensional system is studied within leading-order perturbation theory. We find that the wave-vector dependence of screening in the electron-phonon coupling strength may give rise to a ω³lnω term in the electronic self-energy at zero temperature, where ω is the electronic energy relative to the Fermi energy. Implications of such anomalous self-energy corrections for the electronic specific heat are explored. We find that at finite temperature the specific heat will have an anomalous T³lnT term in addition to the regular linear T term. The possibility of observing such specific-heat anomalies in actual two-dimensional systems is discussed.
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Grempel et al. (1982) studied this question.
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