Mott Quantum Critical Points at Finite Doping

We demonstrate that a finite-doping quantum critical point (QCP) naturally descends from the existence of a first-order Mott transition in the phase diagram of a strongly correlated material. In a prototypical case of a first-order Mott transition the surface associated with the equation of state for the homogeneous system is folded so that in a range of parameters stable metallic and insulating phases exist and are connected by an unstable metallic branch. Here we show that tuning the chemical potential, the zero-temperature equation of state gradually unfolds. Under general conditions, we find that the Mott transition evolves into a first-order transition between two metals, associated with a phase separation region ending in the finite -doping QCP. This scenario is here demonstrated solving a minimal multiorbital Hubbard model relevant for the iron-based superconductors, but its origin-the splitting of the atomic ground state multiplet by a small energy scale, here Hund's coupling-is much more general. A strong analogy with cuprate superconductors is traced.

Automated summary

We demonstrate the existence of a finite-doping quantum critical point (QCP) arising from a first-order Mott transition in the phase diagram of a strongly correlated material. By tuning the chemical potential, we find that the Mott transition evolves into a first-order transition between two metals, leading to a phase separation region ending in the finite-doping QCP. This scenario, demonstrated using a minimal multiorbital Hubbard model, has implications beyond iron-based superconductors and shows a strong analogy with cuprate superconductors.