Magnetic phase diagram of the Hubbard model in the Lieb lattice
arXiv:1505.00578 · doi:10.1016/j.jmmm.2015.02.005
Abstract
We study the mean-field phase diagram of the repulsive Hubbard model in the Lieb lattice. Far from half-filling, the most stable phases are paramagnetism for low on-site interaction and ferromagnetism for high , as in the case of the mean-field phase diagram of the square lattice Hubbard model obtained by Dzierzawa [\onlinecite{Dzierzawa1992}]. At half-filling, the ground state was found to be ferrimagnetic [a spiral phase], in agreement with a theorem by Lieb [\onlinecite{Lieb1989}]. The total magnetization approaches Lieb's prediction as becomes large. As we move away from half-filling, this ferrimagnetic phase becomes a spiral phase with and then undergoes a series of first-order phase transitions, , with , before becoming ferromagnetic at large or paramagnetic at low .
arXiv comment6 pages, 5 figures
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- Ground state spin and excitation energies in half-filled Lieb lattices
- Canted magnetism and fractionalization in metallic states of the Lieb lattice Hubbard model near quarter filling
- Surface magnon spectra of nodal loop semimetals
- Update of Hartree--Fock theory for Hubbard-like models