Abstract

The charge–spin response thermodynamics in the presence of a magnetic field are calculated using analytical diagonalization of small clusters. Rigorous criteria for the Mott–Hubbard, Néel and zero-field (spin) weak pseudogap singularities ( crossovers) in the thermodynamic charge and spin density of states are found for the first time in the exactly solvable two- and four-site Hubbard ( U ⩾ 0 ) clusters. These exact calculations of the chemical potential, magnetization, charge and spin susceptibilities show the presence of true Mott–Hubbard (charge), antiferromagnetic (spin) and zero-field (spin) ground state gaps and pseudogaps that develop at infinitesimal temperatures. These pseudogaps exist in a limited range of temperature or/and doping levels and disappear at the critical temperatures of crossovers ( bifurcations), reminiscent of the pseudogaps and normal-state phase diagram in the high T c cuprates.

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