Abstract
We investigate superconductivity in a two-orbital Hubbard model on a square lattice by applying fluctuation exchange approximation. In the present model, the symmetry of the two orbitals are assumed to be that of an orbital. Then, we find that an -wave spin-triplet orbital-antisymmetric state and a -wave spin-singlet orbital-antisymmetric state appear when Hund’s rule coupling is large. These states are prohibited in a single-orbital model within states with even frequency dependence, but allowed for multiorbital systems. We also discuss pairing symmetry in other models which are equivalent to the two-orbital Hubbard model except for symmetry of orbitals. Finally, we show that pairing states with a finite total momentum, even without a magnetic field, are possible in a system with two Fermi surfaces.
- Received 26 December 2006
DOI:https://doi.org/10.1103/PhysRevB.75.224509
©2007 American Physical Society