Bose metal in exactly solvable model with infinite-range Hatsugai-Kohmoto interaction

TL;DR

This paper demonstrates the realization of a Bose metal state in an exactly solvable model with infinite-range Hatsugai-Kohmoto interactions, revealing a new phase distinct from insulators and superfluids.

Contribution

It introduces an exactly solvable bosonic model extending the Bose-Hubbard model, showing the existence of a Bose metal state without symmetry breaking.

Findings

Bose metal state exists for a range of parameters in the BHK model.

Quantum phase transition between Mott insulator and Bose metal is Lifshitz type.

Finite temperature behavior of the Bose metal resembles a Fermi liquid.

Abstract

In a conventional boson system, the ground state can either be an insulator or a superfluid (SF) due to the duality between particle number and phase. This paper reveals that the long-sought Bose metal (BM) state can be realized in an exactly solvable interacting bosonic model, i.e. the Bose-Hatsugai-Kohmoto (BHK) model, which acts as the nontrivial extension of Bose-Hubbard (BH) model. By tuning the parameters such as bandwidth $W$, chemical potential $\mu$, and interaction strength $U$, a BM state without any symmetry-breaking can be accessed for a generic $W/U$ ratio, while a Mott insulator (MI) with integer boson density is observed at small $W/U$. The quantum phase transition between the MI and BM states belongs to the universality class of the Lifshitz transition, which is further confirmed by analyzing the momentum-distribution function, the Drude weight, and the superfluid density. Additionally, our investigation at finite temperature reveals similarities between the BM state and the Fermi liquid, such as a linear-$T$ dependent heat capacity ($Cv\sim \gamma T$) and a saturated charge susceptibility ($\chi_{c} \sim $ constant) as $T$ approaches zero. Comparing the BM state with the SF state in the standard BH model, we find that the key feature of the BM state is a compressible total wavefunction accompanied by an incompressible zero-momentum component. Given that the BM state prevails over the SF state at any finite $U$ in the BHK model, our work suggests the possibility of realizing the BM state with on-site repulsion interactions in momentum space.