Hubbard model on an anisotropic checkerboard lattice at finite temperatures: Magnetic and metal–insulator transitions
Liu Hai-Di †
Density of states at different interaction strengths with (a) T=0.05, t2=0, (b) T=0.05, t2=0.2, (c) T=0.05, t2=0.5, and (d) T=0.1, t2=0.5. The frequency ω (which is also the energy, because we set the reduced Planck constant to unity) is counted from the chemical potential.