SO4 SYMMETRY IN A HUBBARD MODEL

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Abstract
For a simple Hubbard model, using a particle-particle pairing operator η and a particle-hole pairing operator ζ, it is shown that one can write down two commuting sets of angular momenta operators J and J′, both of which commute with the Hamiltonian. These considerations allow the introduction of quantum numbers j and j′, and lead to the fact that the system has SO 4 = ( SU 2 × SU 2)/ Z 2 symmetry. j is related to the existence of superconductivity for a state and j′ to its magnetic properties.

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