Dynamical critical exponent of the Jaynes-Cummings-Hubbard model

Details Dynamical critical exponent of the Jaynes-Cummings-Hubbard model Dynamical critical exponent of the Jaynes-Cummings-Hubbard model

2011-06-04

arxiv.org/abs/1106.0801v2

Phys. Rev. A 84, 041608(R) (2011)

Physics

Condensed Matter

Strongly Correlated Electrons

4 pages, 4 figures. To appear as a Rapid Communication in Phys. Rev. A

Scientific paper

10.1103/PhysRevA.84.041608

An array of high-Q electromagnetic resonators coupled to qubits gives rise to the Jaynes-Cummings-Hubbard model describing a superfluid to Mott insulator transition of lattice polaritons. From mean-field and strong coupling expansions, the critical properties of the model are expected to be identical to the scalar Bose-Hubbard model. A recent Monte Carlo study of the superfluid density on the square lattice suggested that this does not hold for the fixed-density transition through the Mott lobe tip. Instead, mean-field behavior with a dynamical critical exponent z=2 was found. We perform large-scale quantum Monte Carlo simulations to investigate the critical behavior of the superfluid density and the compressibility. We find z=1 at the tip of the insulating lobe. Hence the transition falls in the 3D XY universality class, analogous to the Bose-Hubbard model.

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