Rigorous bounds on the susceptibilities of the single-band Hubbard model which hold in all dimensions are presented. In the attractive model the spin susceptibility is bounded above by (4{}U{})^-1 where U(0) is the on-site interaction potential. In the half-filled repulsive model on a bipartite lattice the charge and the on-site pairing susceptibilities are bounded above by U^-1. The present result implies that the susceptibilities never diverge in the above mentioned circumstances and also the absence of corresponding long-range order.
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Kubo et al. (1990) studied this question.
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