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The effective Hamiltonian, obtained from the Hubbard model in the strong-coupling limit, is diagonalized exactly for a periodic two-dimensional square lattice of ten sites. We obtain the ground state of the system for any filling of the lattice and the k-space excitation spectrum for a single hole. Within our finite-size system, it is found that for very small coupling ratio t/U, each hole creates a local ferromagnetic environment at least of the size of our system, whereas for increasing t/U, the holes tend to form clusters, induced by antiferromagnetic spin correlations. A range of t/U exists for which pairing of the holes may be possible.
©1988 The American Physical Society.
PACS: 75.10.Jm 74.20.-z
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