Abstract

We study the strong-coupling limit of a two-band Hubbard Hamiltonian that includes an interorbital on-site repulsive interaction ${U}_{ab}$. When the two bands have opposite parity and are quarter filled, we prove that the ground state is simultaneously ferromagnetic and ferroelectric for intraorbital Coulomb interactions ${U}_{aa},{U}_{bb}\ensuremath{\gg}{U}_{ab}$. We also show that this coexistence leads to an enormous magnetoelectric effect.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call