Abstract
An effective Hamiltonian for the two-band Hubbard model was derived by a canonical transformation which was calculated and summed up to infinite order. The transformed Hamiltonian contains terms with strongly renormalized interaction energies. These new interaction energies show sign reversals as a function of the hopping integral in addition to a strong reduction in the charge-transfer gap and a significant increase in the attractive oxygen Hubbard term.
Original language | English |
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Pages (from-to) | 671-680 |
Number of pages | 10 |
Journal | Philosophical Magazine Letters |
Volume | 82 |
Issue number | 12 |
DOIs | |
Publication status | Published - Dec 2002 |