Quantum criticality of a Bose gas in an optical lattice near the Mott transition
arXiv:1107.1314 · doi:10.1103/PhysRevA.85.011602
Abstract
We derive the equation of state of bosons in an optical lattice in the framework of the Bose-Hubbard model. Near the density-driven Mott transition, the expression of the pressure P(μ,T) versus chemical potential and temperature is similar to that of a dilute Bose gas but with renormalized mass m^* and scattering length a^*. m^* is the mass of the elementary excitations at the quantum critical point governing the transition from the superfluid phase to the Mott insulating phase, while a^* is related to their effective interaction at low energy. We use a nonperturbative renormalization-group approach to compute these parameters as a function of the ratio t/U between hopping amplitude and on-site repulsion.
v1) 4 pages, 6 figures. v2) Significant rewriting (new title) with more emphasis on the quantum critical behavior near the Mott transition
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- Renormalization group study of Bose polarons
- Thermodynamics of a Bose gas near the superfluid--Mott-insulator transition
- A Non-Perturbative Renormalization Group approach to quantum XY spin models
- Nonperturbative functional renormalization-group approach to transport in the vicinity of a -dimensional O()-symmetric quantum critical point
- Quantum XY criticality in a two-dimensional Bose gas near the Mott transition
- Strong-coupling RPA theory of a Bose gas near the superfluid--Mott-insulator transition: universal thermodynamics and two-body contact
- Two-body contact of a Bose gas near the superfluid--Mott-insulator transition