The temperature and doping dependence of the 2D Hubbard model is studied in
the intermediate coupling regime (U = 4). Strong 2D critical spin fluctuat
ions dominating near half-filling are completely destroyed upon about 14% d
oping concentration, below which the imaginary part of the self-energy vani
shes nearly quadratically in both frequency and temperature, a characterist
ic feature for the Fermi liquid. As the doping concentration is increased f
rom half-filling, dynamical spin susceptibility shows a change from commens
urate to incommensurate structure, leading to a three-peak structure in the
spectral function in some region of the Brillouin zone. (C) 1999 Elsevier
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