Antiferromagnetic spin fluctuations in a two-dimensional metal, such as doped high-Tc superconductors, lead to a pseudogap in the electronic spectrum. In the spectral function weight is shifted from the single quasiparticle peak of the Fermi-liquid regime to the incoherent particle and hole backgrounds, which evolve into the upper and lower Mott-Hubbard bands of the antiferromagnetic insulator. Precursors of these split bands show up as ``shadow bands'' in angle-resolved photoemission spectra.
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Kampf et al. (1990) studied this question.
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