Abstract
By exploiting the particle-hole symmetries of the Hubbard model, the periodic Anderson model, and the Kondo lattice model at half-filling and by applying a generalized version of Lieb's spin-reflection positivity method, we show that the charged gaps of these models are always larger than their spin-excitation gaps. This theorem confirms the previous results derived by either the variational approach or the density-matrix renormalization-group approach.
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