Anderson localization in the Anderson-Hubbard model with site-dependent interactions

We consider Anderson localization in the half-filled Anderson-Hubbard model in the presence of either random on-site interactions or spatially alternating interactions in the lattice. By using dynamical mean field theory with the equation of motion method as an impurity solver, we calculate the arithmetically and geometrically averaged local density of states and derive the equations determining the critical value for the phase transition between metallic, Anderson and Mott insulating phases. The nonmagnetic ground state phase diagrams are constructed numerically. We figure out that the presence of Coulomb disorder drives the system toward the Anderson localized phase that can occur even in the absence of Anderson structural disorder. For the spatially alternating interactions, we find that the metallic region is reduced and the Anderson insulator one is enlarged with increasing interaction modulation. Our obtained results are relevant to current research in ultracold atoms in disordered optical lattices where metal-insulator transition can be observed experimentally by using ultracold atom techniques.

Automated summary

In this study, we investigate Anderson localization in the half-filled Anderson-Hubbard model with random on-site interactions or spatially alternating interactions. By using dynamical mean field theory and the equation of motion method as an impurity solver, we calculate the arithmetically and geometrically averaged local density of states and derive the equations determining the critical value for the phase transition between metallic, Anderson and Mott insulating phases. The nonmagnetic ground state phase diagrams are constructed numerically, and we observe that Coulomb disorder drives the system towards Anderson localization phase even without Anderson structural disorder. Additionally, for spatially alternating interactions, we find that increasing interaction modulation reduces the metallic region and enlarges the Anderson insulator region. These findings are relevant to the study of ultracold atoms in disordered optical lattices and can be experimentally observed using ultracold atom techniques.