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We investigate the effect of doping in the hole spectral function by exact diagonalization of a 16-site cluster with two holes. It is shown that for more than one hole the spectral function differs qualitatively from the one in the single-hole limit. In particular, we find no evidence for the formation of a Fermi surface having hole ``pockets'' localized around (±{}{π}/2,±{}{π}/2) in momentum space. On the contrary, a large low-energy peak appears in the spectral function of the hole propagator at k=({π},0) or (0,{π}) which is then the best candidate for the existence of those pockets. A ({π}/2,{π}/2) quasihole state is obtained as a small energy excitation of the two-hole system. We discuss some consequences for photoemission and optical-conductivity experiments in high-Tc materials at intermediate doping.
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Poilblanc et al. (1990) studied this question.
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