By subdividing a 2d square lattice into plaquettes containing 4 lattice sit
es each, the Hubbard Hamiltonian is reformulated in terms of different "col
ored" fermion species. This makes it possible to describe e.g. antiferromag
netic order or d-wave superconductivity in terms of expectation values of c
omposite scalar fields. A suitable mean field approximation indeed reproduc
es qualitatively the measured phase diagram and shows a competition between
phases with antiferromagnetic ordering and d(x2-y2)-superconductivity at l
ow temperatures.