Two Theorems on Pseudo-spin in the Hubbard Model
arXiv:cond-mat/9911163 · doi:10.1016/S0375-9601(00)00042-6
Abstract
An inequality of the eigenvalues of the reduced density matrix at finite temperature in the Hubbard model is obtained by means of the Bogolyubov inequality. The quasi-average of in a simple symmetry-breaking perturbation of the Hamiltonian for a bipartite lattice is shown to be zero.
8 pages, LATEX, no figures