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The energy spectrum of the one-dimensional electron gas, solved by Luther and Emery for a particular attractive interaction strength U of the backward scattering across the Fermi surface, has been calculated for small deviations from this particular limit. The energy spectrum shows a gap at the Fermi energy, whose magnitude is very sensitive to the interaction U. The density of states shows a gap at zero temperature, which is smeared out by the quasiparticle lifetime for T≠0.
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P. Schlottmann (1977) studied this question.
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